JP2010195327A - Device and method for estimating tread friction state of vehicle - Google Patents

Device and method for estimating tread friction state of vehicle Download PDF

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JP2010195327A
JP2010195327A JP2009044861A JP2009044861A JP2010195327A JP 2010195327 A JP2010195327 A JP 2010195327A JP 2009044861 A JP2009044861 A JP 2009044861A JP 2009044861 A JP2009044861 A JP 2009044861A JP 2010195327 A JP2010195327 A JP 2010195327A
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road surface
force
tire
slip
wheel
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JP5206491B2 (en
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Hiroki Shiozawa
裕樹 塩澤
Masaaki Nawano
昌明 縄野
Hiroshi Mori
宏 毛利
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Nissan Motor Co Ltd
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Abstract

<P>PROBLEM TO BE SOLVED: To provide a device and method for estimating a road surface μ before the occurrence of slip. <P>SOLUTION: The device for estimating a tread friction state of a vehicle detects a resultant force composed of a braking force and a lateral force of a wheel, and a slippage of the wheel (steps S21 and S22); and calculates a road surface friction factor of a current road surface based on a distance obtained by projecting, in a three-dimensional space having the braking force, lateral force and slippage of the wheel as coordinate axes, the magnitude of a current tire force to a line extending from an origin where the braking force, lateral force and slippage are zero to the detected current slippage in the direction of the detected current tire force (steps S23 and S24). <P>COPYRIGHT: (C)2010,JPO&INPIT

Description

本発明は、車両の車輪の接地面グリップ特性を推定する技術に関する。   The present invention relates to a technique for estimating a ground contact surface grip characteristic of a vehicle wheel.

走行制御装置として、駆動輪の回転速度を計測し、その回転角加速度の最大値から路面μを推定し、駆動輪にスリップが発生しないよう最適なトルク制御を行う装置がある(例えば特許文献1参照)。   As a travel control device, there is a device that measures the rotational speed of driving wheels, estimates the road surface μ from the maximum value of the rotational angular acceleration, and performs optimal torque control so that slip does not occur on the driving wheels (for example, Patent Document 1). reference).

特公平6−78736号公報Japanese Examined Patent Publication No. 6-78736

しかしながら、この装置では、駆動輪の回転速度から路面μを推定しているために、駆動輪に実際にスリップが発生しないと、路面μを判別することができない。これでは、スリップにより制駆動力のロスが発生し、車両旋回中では、スピンやドリフトアウトしてしまう場合がある。
本発明の課題は、スリップが発生する前に走行路面の路面μを推定することである。
However, in this apparatus, since the road surface μ is estimated from the rotational speed of the drive wheel, the road surface μ cannot be determined unless slip actually occurs in the drive wheel. This causes a loss of braking / driving force due to the slip, and may spin or drift out while the vehicle is turning.
An object of the present invention is to estimate the road surface μ of the traveling road surface before slip occurs.

前記課題を解決するために、本発明は、現在のタイヤ力、現在のスリップ度及びタイヤ特性相関関係マップを基に、現在の路面の路面摩擦係数を算出する。
タイヤ特性相関関係マップは、基準路面摩擦係数の基準路面で得られる車輪の制駆動力、車輪の横力及び車輪のスリップ度の相関関係で成立する3次元曲面を表すタイヤ特性をモデル化したものであり、基準路面での制駆動力と横力との合力とスリップ度との比と基準路面摩擦係数とは異なる路面摩擦係数の路面での制駆動力と横力との合力とスリップ度との比が同一であれば、基準路面での制駆動力と横力との合力と、基準路面摩擦係数とは異なる路面摩擦係数の路面での制駆動力と横力との合力との比、又は基準路面でのスリップ度と、基準路面摩擦係数とは異なる路面摩擦係数の路面でのスリップ度との比が、基準路面摩擦係数と、基準路面摩擦係数とは異なる路面摩擦係数との比を示す特性を有する。
In order to solve the above problems, the present invention calculates a road surface friction coefficient of a current road surface based on a current tire force, a current slip degree, and a tire characteristic correlation map.
The tire characteristic correlation map is a model of tire characteristics representing a three-dimensional curved surface established by the correlation between the braking / driving force of the wheel, the lateral force of the wheel, and the slip degree of the wheel obtained on the reference road surface of the reference road surface friction coefficient. The ratio of the resultant force between the braking / driving force and lateral force on the reference road surface and the slip ratio and the resultant force and the slip force on the road surface with a road surface friction coefficient different from the reference road friction coefficient If the ratio is the same, the ratio of the resultant force of braking / driving force and lateral force on the reference road surface to the resultant force of braking / driving force and lateral force on the road surface with a road surface friction coefficient different from the reference road friction coefficient, Alternatively, the ratio between the slip degree on the reference road surface and the slip degree on the road surface with a road surface friction coefficient different from the reference road surface friction coefficient is the ratio between the reference road surface friction coefficient and the road surface friction coefficient different from the reference road surface friction coefficient. It has the characteristics shown.

本発明は、このような特性を有するタイヤ特性相関関係マップを用いて、車輪の制駆動力、車輪の横力及び車輪のスリップ度を座標軸とする3次元空間における、該制動力、横力及びスリップ度が零である原点から、検出ステップで検出した現在のタイヤ力の方向でかつ検出ステップで検出した現在のスリップ度まで延びる直線に該現在のタイヤ力の大きさを投影して得た距離と、前記直線を延長してタイヤ特性相関関係マップと交じわる交点と前記原点との間の距離との比を基に、現在の路面の路面摩擦係数を算出する。   The present invention uses a tire characteristic correlation map having such characteristics to use the braking force, lateral force, and lateral force in a three-dimensional space with wheel braking / driving force, wheel lateral force, and wheel slip degree as coordinate axes. Distance obtained by projecting the current tire force magnitude on a straight line extending from the origin where the slip degree is zero to the current tire force direction detected in the detection step and to the current slip degree detected in the detection step Then, the road surface friction coefficient of the current road surface is calculated based on the ratio of the distance between the intersection point intersecting the tire characteristic correlation map by extending the straight line and the origin point.

ここで、車輪の制駆動力、車輪の横力及び車輪のスリップ度を座標軸とする3次元空間でみると、基準路面での制駆動力と横力との合力とスリップ度との比と基準路面摩擦係数とは異なる路面摩擦係数の路面での制駆動力と横力との合力とスリップ度との比が同一であるときに、基準路面での制駆動力と横力との合力と、基準路面摩擦係数とは異なる路面摩擦係数の路面での制駆動力と横力との合力との比、又は基準路面でのスリップ度と、基準路面摩擦係数とは異なる路面摩擦係数の路面でのスリップ度との比と、3次元空間の原点から、検出した現在のタイヤ力の方向でかつ検出した現在のスリップ度まで延びる直線に該現在のタイヤ力の大きさを投影して得た距離と、前記直線を延長してタイヤ特性相関関係マップと交じわる交点と前記原点との間の距離との比とは、幾何学的にみて一致する。   Here, in a three-dimensional space with the wheel braking / driving force, wheel lateral force and wheel slip degree as coordinate axes, the ratio of the resultant force of the braking / driving force and the lateral force on the reference road surface to the slip degree and the reference When the ratio of the resultant force of the braking / driving force and lateral force on the road surface with a road surface friction coefficient different from the road surface friction coefficient and the slip ratio is the same, the resultant force of the braking / driving force and lateral force on the reference road surface, The ratio of the braking / driving force and lateral force on the road surface with a road surface friction coefficient different from the reference road surface friction coefficient, or the slip degree on the reference road surface, and the road surface friction coefficient different from the reference road surface friction coefficient A ratio obtained by projecting the magnitude of the current tire force on a straight line extending from the origin of the three-dimensional space to the detected current tire force direction and to the detected current slip degree; , Extending the straight line and intersecting with the tire characteristic correlation map And the ratio of the distance between the origin is consistent viewed geometrically.

よって、3次元空間の原点から、検出した現在のタイヤ力の方向でかつ検出した現在のスリップ度まで延びる直線に該現在のタイヤ力の大きさを投影して得た距離と、前記直線を延長してタイヤ特性相関関係マップと交じわる交点と前記原点との間の距離との比、及び基準路面摩擦係数から、現在の路面の路面摩擦係数を算出できる。   Therefore, the distance obtained by projecting the magnitude of the current tire force on the straight line extending from the origin of the three-dimensional space to the detected current slip direction in the direction of the detected current tire force, and the straight line extended. Thus, the road surface friction coefficient of the current road surface can be calculated from the ratio of the intersection between the tire characteristic correlation map and the distance between the origin and the reference road surface friction coefficient.

本発明によれば、車輪のタイヤ力の方向及び大きさ、並びにスリップ度を検出して、現在の路面の路面摩擦係数を算出できる。
これにより、スリップが発生する前に現在の路面の路面摩擦係数を推定できる。
According to the present invention, the road surface friction coefficient of the current road surface can be calculated by detecting the direction and magnitude of the tire force of the wheel and the slip degree.
As a result, the road surface friction coefficient of the current road surface can be estimated before slip occurs.

前提となる技術を説明するために使用した図であり、車輪のスリップ率λと車輪の制駆動力Fxとの間に成立するタイヤ特性曲線(Fx−λ特性曲線)を示す特性図である。FIG. 6 is a characteristic diagram showing a tire characteristic curve (Fx-λ characteristic curve) established between a wheel slip ratio λ and a wheel braking / driving force Fx, which is used for explaining a presupposed technology. 前提となる技術を説明するために使用した図であり、各路面μのタイヤ特性曲線(Fx−λ特性曲線)及び摩擦円を示す特性図である。It is a figure used in order to explain a premise technique, and is a characteristic view showing a tire characteristic curve (Fx-λ characteristic curve) and a friction circle of each road surface μ. 前提となる技術を説明するために使用した図であり、各路面μのタイヤ特性曲線(Fx−λ特性曲線)について、該タイヤ特性曲線の原点を通る直線との交点での接線の傾きを示す特性図である。It is the figure used in order to explain the premise technology, and shows the inclination of the tangent at the intersection of the tire characteristic curve (Fx-λ characteristic curve) of each road surface μ and the straight line passing through the origin of the tire characteristic curve FIG. 前提となる技術を説明するために使用した図であり、各路面μのタイヤ特性曲線(Fx−λ特性曲線)について、該タイヤ特性曲線の原点を通る直線との交点での接線の傾きを示す他の特性図である。It is the figure used in order to explain the premise technology, and shows the inclination of the tangent at the intersection of the tire characteristic curve (Fx-λ characteristic curve) of each road surface μ and the straight line passing through the origin of the tire characteristic curve It is another characteristic view. 前提となる技術を説明するために使用した図であり、路面μが異なるタイヤ特性曲線について得られる制駆動力Fx同士の比、スリップ率λ同士の比、又は線長同士の比と、路面μの比とが等しくなることを示す特性図である。It is the figure used in order to explain the technology which is the premise, the ratio of braking / driving force Fx, the ratio of slip ratios λ, or the ratio of line lengths and road surface μ obtained for tire characteristic curves with different road surface μ It is a characteristic view which shows that the ratio of becomes equal. 前提となる技術を説明するために使用した図であり、制駆動力Fx及びスリップ率λから得た線長同士の比を基に路面μを算出する手順を示す図である。It is a figure used in order to explain a premise technique, and is a figure showing a procedure which calculates road surface μ based on a ratio of line lengths obtained from braking / driving force Fx and slip rate λ. 前提となる技術を説明するために使用した図であり、路面μが異なる路面で得た制駆動力Fxとスリップ率λとの関係を示す特性図である。FIG. 5 is a characteristic diagram showing the relationship between braking / driving force Fx and slip ratio λ obtained on road surfaces with different road surface μ, which is used to explain the underlying technology. 前提となる技術を説明するために使用した図であり、スタッドレスタイヤについて、路面μが異なる路面で得た制駆動力Fxとスリップ率λとの関係を示す特性図である。It is a figure used in order to explain the technology used as a premise, and is a characteristic view showing the relation between braking / driving force Fx and slip ratio λ obtained on road surfaces with different road surface μ for studless tires. 前提となる技術を説明するために使用した図であり、タイヤ特性曲線(Fx−λ特性曲線)の任意点の制駆動力Fxとスリップ率λとの比(Fx/λ)と、その任意点でのタイヤ特性曲線の接線の傾き(μ勾配)とのプロット点の集合からなる特性図である。It is the figure used in order to explain the premise technology, ratio (Fx / λ) of braking / driving force Fx and slip ratio λ of the arbitrary point of the tire characteristic curve (Fx-λ characteristic curve) and the arbitrary point FIG. 6 is a characteristic diagram composed of a set of plot points with a slope (μ gradient) of a tangent line of a tire characteristic curve in FIG. 前提となる技術を説明するために使用した図であり、図9のプロット点から得た特性曲線(グリップ特性曲線)を示す特性図である。FIG. 10 is a characteristic diagram showing a characteristic curve (grip characteristic curve) obtained from the plotted points in FIG. 車輪のスリップ角βtと車輪の横力Fyとの間に成立するタイヤ特性曲線(Fy−βt特性曲線)を示す特性図である。FIG. 5 is a characteristic diagram showing a tire characteristic curve (Fy-βt characteristic curve) established between a wheel slip angle βt and a wheel lateral force Fy. 前提となる技術を説明するために使用した図であり、各路面μのタイヤ特性曲線(Fy−βt特性曲線)及び摩擦円を示す特性図である。It is a figure used in order to explain a premise technique, and is a characteristic figure showing a tire characteristic curve (Fy-βt characteristic curve) and a friction circle of each road surface μ. 前提となる技術を説明するために使用した図であり、各路面μのタイヤ特性曲線(Fy−βt特性曲線)について、該タイヤ特性曲線の原点を通る直線との交点での接線の傾きを示す特性図である。It is the figure used in order to explain the premise technology, and shows the inclination of the tangent at the intersection of the tire characteristic curve (Fy-βt characteristic curve) of each road surface μ and the straight line passing through the origin of the tire characteristic curve FIG. 前提となる技術を説明するために使用した図であり、各路面μのタイヤ特性曲線(Fy−βt特性曲線)について、該タイヤ特性曲線の原点を通る直線との交点での接線の傾きを示す他の特性図である。It is the figure used in order to explain the premise technology, and shows the inclination of the tangent at the intersection of the tire characteristic curve (Fy-βt characteristic curve) of each road surface μ and the straight line passing through the origin of the tire characteristic curve It is another characteristic view. 前提となる技術を説明するために使用した図であり、路面μが異なるタイヤ特性曲線について得られる横力Fy同士の比、スリップ角βt同士の比、又は線長同士の比と、路面μの比とが等しくなることを示す特性図である。It is the figure used in order to explain the technology which is the premise, ratio of the lateral forces Fy which are obtained about the tire characteristic curve where road surface μ differs, ratio of slip angle βt or ratio of line length and road surface μ It is a characteristic view which shows that ratio becomes equal. 前提となる技術を説明するために使用した図であり、横力Fy及びスリップ角βtから得た線長同士の比を基に路面μを算出する手順を示す図である。It is a figure used in order to explain the technology used as a premise, and is a figure which shows the procedure which calculates road surface (micro | micron | mu) based on ratio of the line length obtained from lateral force Fy and slip angle (beta) t. 前提となる技術を説明するために使用した図であり、路面μが異なるタイヤ特性曲線について得られるタイヤ力F同士の比、スリップ度S同士の比、又は線長同士の比と、路面μの比とが等しくなることを示す特性図である。It is the figure used in order to explain the technology which is the premise, the ratio of tire force F which is obtained about the tire characteristic curve where road surface μ differs, ratio of slip degree S or ratio of line length and road surface μ It is a characteristic view which shows that ratio becomes equal. 前提となる技術を説明するために使用した図であり、タイヤ特性曲線(Fy−βt特性曲線)の任意点の横力Fyとスリップ角βtとの比(Fy/βt)と、その任意点でのタイヤ特性曲線の接線の傾き(μ勾配)との関係(グリップ特性曲線)を示す特性図である。It is the figure used in order to explain a premise technique, and is a ratio (Fy / βt) of lateral force Fy and slip angle βt of an arbitrary point of a tire characteristic curve (Fy-βt characteristic curve), and the arbitrary point It is a characteristic view which shows the relationship (grip characteristic curve) with the inclination (micro gradient) of the tangent of the tire characteristic curve. 前提となる技術を説明するために使用した図であり、制駆動力(前後力)Fxを第1軸、横力Fyを第2軸上で表現する直交座標面上に摩擦円を表現した特性図である。It is the figure used in order to explain the premise technology, the characteristic which expressed the friction circle on the orthogonal coordinate plane which expresses braking / driving force (front / rear force) Fx on the 1st axis and lateral force Fy on the 2nd axis FIG. 前提となる技術において制駆動力Fxとスリップ率λとの関係を3次元座標系に表示する手順を説明するために使用した図であり、制駆動力Fxとスリップ率λとの関係を示す特性図である。FIG. 5 is a diagram used to explain the procedure for displaying the relationship between braking / driving force Fx and slip rate λ in a three-dimensional coordinate system in the premise technology, and shows the relationship between braking / driving force Fx and slip rate λ FIG. 前提となる技術において横力Fyとスリップ角βtとの関係を3次元座標系に表示する手順を説明するために使用した図であり、横力Fyとスリップ角βtとの関係を示す特性図である。It is a figure used in order to demonstrate the procedure which displays the relationship between lateral force Fy and slip angle (beta) t in a three-dimensional coordinate system in a premise technique, and is a characteristic view which shows the relationship between lateral force Fy and slip angle (beta) t. is there. 前提となる技術において車輪力(制駆動力Fx、横力Fy)とスリップ度(スリップ率λ、スリップ角βt)との関係を3次元座標系に表示する手順を説明するために使用した図であり、3次元曲面で車輪力(制駆動力Fx、横力Fy)とスリップ度(スリップ率λ、スリップ角βt)との関係を示す特性図である。FIG. 5 is a diagram used to explain the procedure for displaying the relationship between wheel force (braking / driving force Fx, lateral force Fy) and slip degree (slip rate λ, slip angle βt) in a three-dimensional coordinate system in the underlying technology. FIG. 5 is a characteristic diagram showing the relationship between wheel force (braking / driving force Fx, lateral force Fy) and slip degree (slip rate λ, slip angle βt) on a three-dimensional curved surface. 前提となる技術を説明するために使用した図である。(a)は、スリップ度と車輪力との関係を表す3次元曲面と制駆動力Fxと横力Fyとの合力FのベクトルとZ軸とを含む平面との交線を示す特性図である。(b)は、合力Fと合力Fに起因して発生するスリップ度Zとの関係を示すタイヤ特性曲線(F−Z特性曲線)を示す特性図である。It is the figure used in order to demonstrate the technique used as a premise. (A) is a characteristic diagram showing an intersection line between a three-dimensional curved surface representing the relationship between the slip degree and the wheel force, a vector of the resultant force F of the braking / driving force Fx and the lateral force Fy, and a plane including the Z axis. . (B) is a characteristic diagram showing a tire characteristic curve (FZ characteristic curve) showing a relationship between the resultant force F and the slip degree Z generated due to the resultant force F. FIG. 前提となる技術を説明するために使用した図である。(a)は、3次元座標系においてタイヤ摩擦円の大きさの違いを示す特性図である。(b)は、摩擦円の大きさを決める最大摩擦力の大きさの違いによるタイヤ特性曲線(F−Z特性曲線)の変化を示すための特性図である。It is the figure used in order to demonstrate the technique used as a premise. (A) is a characteristic view showing a difference in size of a tire friction circle in a three-dimensional coordinate system. (B) is a characteristic diagram for showing a change in the tire characteristic curve (FZ characteristic curve) due to the difference in the magnitude of the maximum frictional force that determines the size of the friction circle. 前提となる技術を説明するために使用した図である。(a)は、タイヤ特性曲線と原点0(スリップ度と車輪力がともに0である点)を通る直線との交点における傾きが、最大摩擦力の大きさによらず一定の値となることを示す3次元座標系の特性図である。(b)は、タイヤ特性曲線と原点0を通る直線との交点における傾きが、最大摩擦力の大きさによらず一定の値となることを示す2次元座標系の特性図である。It is the figure used in order to demonstrate the technique used as a premise. (A) shows that the slope at the intersection of the tire characteristic curve and a straight line passing through the origin 0 (a point where both the slip degree and the wheel force are 0) has a constant value regardless of the magnitude of the maximum frictional force. It is a characteristic view of the three-dimensional coordinate system shown. (B) is a characteristic diagram of a two-dimensional coordinate system showing that the slope at the intersection of the tire characteristic curve and a straight line passing through the origin 0 is a constant value regardless of the magnitude of the maximum frictional force. 前提となる技術を説明するために使用した図であり、路面μが異なる各タイヤ特性曲線(F−Z特性曲線)について、合力F同士の比又はスリップ度Z同士の比と、その路面μの比とが等しくなることを示す特性図である。It is the figure used in order to explain the technology which becomes the premise, for each tire characteristic curve (FZ characteristic curve) where road surface μ differs, ratio of resultant force F or ratio of slip degree Z and the road surface μ It is a characteristic view which shows that ratio becomes equal. 前提となる技術を説明するために使用した図であり、合力F及びスリップ度Sから得た線長同士の比を基に路面μを算出する手順を示す図である。It is a figure used in order to explain the technology used as a premise, and is a figure which shows the procedure which calculates road surface (micro | micron | mu) based on ratio of the line length obtained from resultant force F and slip degree S. FIG. 前提となる技術を説明するために使用した図であり、タイヤ特性曲線(F−Z特性曲線)の任意点の合力Fとスリップ度Zとの比(F/Z)と、その任意点でのタイヤ特性曲線の接線の傾き(μ勾配)との関係(グリップ特性曲線)を示す特性図である。It is the figure used in order to explain the technology used as a premise, the ratio (F / Z) of the resultant force F and the slip degree Z of the arbitrary point of a tire characteristic curve (FZ characteristic curve), and the arbitrary point FIG. 5 is a characteristic diagram showing a relationship (grip characteristic curve) with a tangential slope (μ gradient) of a tire characteristic curve. 実施形態の車両の概略構成を示す図である。It is a figure showing a schematic structure of a vehicle of an embodiment. 車両走行状態推定装置の構成を示すブロック図である。It is a block diagram which shows the structure of a vehicle running state estimation apparatus. 車体スリップ角推定部の構成を示すブロック図である。It is a block diagram which shows the structure of a vehicle body slip angle estimation part. 旋回中の車体に働く場の力を説明するために使用した図である。It is the figure used in order to explain the field force which acts on the body during turning. 旋回中の車体に働く場の力を説明するために使用した図である。It is the figure used in order to explain the field force which acts on the body during turning. 補償ゲインを設定するための制御マップを説明するために使用した特性図である。It is the characteristic view used in order to demonstrate the control map for setting a compensation gain. 車両の線形2輪モデルを説明するために使用した図である。It is the figure used in order to explain the linear two-wheel model of vehicles. 3D特性マップを示す図である。It is a figure which shows 3D characteristic map. 3D特性マップを参照して路面μを算出する手順を説明するために使用した図である。It is the figure used in order to demonstrate the procedure which calculates road surface micro | micron | mu with reference to a 3D characteristic map. 動作の説明に使用したフローチャートである。It is the flowchart used for description of operation | movement.

以下、本発明の実施形態を図面に基づいて説明する。
(実施形態の前提となる技術)
先ず、本実施形態の前提となる技術を説明する。
(1)車輪のスリップ率と車輪の制駆動力との関係
図1はタイヤ特性曲線を示す。このタイヤ特性曲線は、駆動輪のスリップ率λと駆動輪の制駆動力(又は前後力)Fxとの間に成立する一般的な相関関係を示す。例えば、マジックフォーミュラ(MagicFormula)といったタイヤモデルからタイヤ特性曲線を得る。ここで、制駆動力Fxは、タイヤから地面に作用する力である。また、制駆動力Fxが接地面において車輪に作用する車輪力に相当する。車輪のスリップ率λが車輪のスリップ度に相当する。
Hereinafter, embodiments of the present invention will be described with reference to the drawings.
(Technology that is the premise of the embodiment)
First, a technique that is a premise of the present embodiment will be described.
(1) Relationship between wheel slip ratio and wheel braking / driving force FIG. 1 shows a tire characteristic curve. This tire characteristic curve shows a general correlation established between the slip ratio λ of the drive wheel and the braking / driving force (or longitudinal force) Fx of the drive wheel. For example, a tire characteristic curve is obtained from a tire model such as MagicFormula. Here, the braking / driving force Fx is a force acting on the ground from the tire. The braking / driving force Fx corresponds to the wheel force acting on the wheel on the ground contact surface. The slip ratio λ of the wheel corresponds to the slip degree of the wheel.

図1に示すように、タイヤ特性曲線では、スリップ率λと制駆動力Fxとの関係が、スリップ率λの絶対値が増加するに従い線形(直線関係)から非線形(曲線関係)に遷移する。すなわち、タイヤ特性曲線では、スリップ率λが零から所定の範囲内にある場合には、スリップ率λと制駆動力Fxとの間に線形関係が成り立つ。そして、タイヤ特性曲線では、スリップ率λ(絶対値)がある程度大きくなると(前記所定の範囲を超えると)、スリップ率λと制駆動力Fxとの関係が非線形関係になる。このように、タイヤ特性曲線は、線形部分と非線形部分とを有する。   As shown in FIG. 1, in the tire characteristic curve, the relationship between the slip ratio λ and the braking / driving force Fx changes from linear (linear relationship) to non-linear (curve relationship) as the absolute value of the slip rate λ increases. That is, in the tire characteristic curve, when the slip ratio λ is within a predetermined range from zero, a linear relationship is established between the slip ratio λ and the braking / driving force Fx. In the tire characteristic curve, when the slip ratio λ (absolute value) increases to some extent (exceeding the predetermined range), the relationship between the slip ratio λ and the braking / driving force Fx becomes a non-linear relationship. Thus, the tire characteristic curve has a linear portion and a non-linear portion.

このようなスリップ率λと制駆動力Fxとの間にある関係や線形関係から非線形関係への遷移は、タイヤ特性曲線の接線の傾きに着目すれば一目瞭然である。ここでいうタイヤ特性曲線の接線の傾きとは、スリップ率λの変化量と制駆動力Fxの変化量との比、すなわち、制駆動力Fxのスリップ率λに関する偏微分係数で示される値である。
ここで、図1に示すように、タイヤ特性曲線の原点を通る任意の直線a,b,c,d,…を描く。すると、タイヤ特性曲線に対して交わる任意の直線a,b,c,d,…との交点(同図中に○印で示す交点)でタイヤ特性曲線の接線の傾きを得ることができる。そして、タイヤ特性曲線の接線の傾きは各交点で異なるものとなる。このようなタイヤ特性曲線の接線の傾きに着目することで、スリップ率λと制駆動力Fxとの間にある関係や線形関係から非線形関係への遷移の状態を知ることができる。
Such a transition between the slip ratio λ and the braking / driving force Fx or a transition from a linear relationship to a non-linear relationship is obvious when attention is paid to the slope of the tangent line of the tire characteristic curve. The slope of the tangent line of the tire characteristic curve here is a value indicated by a partial differential coefficient with respect to a ratio of a change amount of the slip ratio λ and a change amount of the braking / driving force Fx, that is, the slip ratio λ of the braking / driving force Fx. is there.
Here, as shown in FIG. 1, arbitrary straight lines a, b, c, d,... Passing through the origin of the tire characteristic curve are drawn. Then, the slope of the tangent line of the tire characteristic curve can be obtained at the intersections with arbitrary straight lines a, b, c, d,. The slope of the tangent line of the tire characteristic curve is different at each intersection. By paying attention to the inclination of the tangent line of the tire characteristic curve, it is possible to know the relationship between the slip ratio λ and the braking / driving force Fx or the state of transition from the linear relationship to the nonlinear relationship.

これにより、タイヤの摩擦状態の推定も可能になる。例えば、図1に示すように、タイヤ特性曲線上で、非線形域でも線形域に近い位置x0にあれば、タイヤの摩擦状態が安定状態にあると推定できる。そして、タイヤの摩擦状態が安定状態にあれば、例えばタイヤがその能力を発揮できるレベルにあると推定できる。又は車両が安定状態にあると推定できる。   Thereby, estimation of the friction state of the tire is also possible. For example, as shown in FIG. 1, if the tire characteristic curve is at a position x0 that is close to the linear region even in the non-linear region, it can be estimated that the tire friction state is in a stable state. And if the friction state of a tire is in a stable state, for example, it can be estimated that the tire is at a level at which its ability can be exhibited. Alternatively, it can be estimated that the vehicle is in a stable state.

図2は、各種路面μのタイヤ特性曲線と摩擦円を示す。図2(a)は、各種路面μのタイヤ特性曲線を示す。図2(b)〜(d)は、各路面μの摩擦円を示す。路面μは例えば0.2、0.5、1.0である。図2(a)に示すように、タイヤ特性曲線は、各路面μで定性的に同様な傾向を示す。また、図2(b)〜(d)に示すように、路面μが小さくなるほど摩擦円が小さくなる。すなわち、路面μが小さくなるほどタイヤが許容できる制駆動力が小さくなる。このように、タイヤ特性は、路面摩擦係数(路面μ)をパラメータとした特性となる。このようなことから、図2に示すように、路面摩擦係数の値に応じて、低摩擦の場合のタイヤ特性曲線、中摩擦の場合のタイヤ特性曲線、及び高摩擦の場合のタイヤ特性曲線等を得ることができる。   FIG. 2 shows tire characteristic curves and friction circles of various road surfaces μ. FIG. 2A shows tire characteristic curves of various road surfaces μ. 2 (b) to 2 (d) show the friction circle of each road surface μ. The road surface μ is, for example, 0.2, 0.5, or 1.0. As shown in FIG. 2 (a), the tire characteristic curve shows the same tendency qualitatively at each road surface μ. Further, as shown in FIGS. 2B to 2D, the friction circle becomes smaller as the road surface μ becomes smaller. That is, the braking / driving force that the tire can tolerate decreases as the road surface μ decreases. As described above, the tire characteristics are characteristics using the road surface friction coefficient (road surface μ) as a parameter. Therefore, as shown in FIG. 2, depending on the value of the road surface friction coefficient, the tire characteristic curve in the case of low friction, the tire characteristic curve in the case of medium friction, the tire characteristic curve in the case of high friction, etc. Can be obtained.

図3は、各種路面μのタイヤ特性曲線と該タイヤ特性曲線の原点を通る任意の直線b,c,dとの関係を示す。図3に示すように、前記図1と同様に、各種路面μのタイヤ特性曲線について、任意の直線b,c,dとの交点で接線の傾きを得る。すなわち、各種路面μでのタイヤ特性曲線について、直線bとの交点で接線の傾きをそれぞれ得る。各種路面μでのタイヤ特性曲線について、直線cとの交点で接線の傾きをそれぞれ得る。各種路面μでのタイヤ特性曲線について、直線dとの交点で接線の傾きをそれぞれ得る。その結果、同一直線との交点で得られる各種路面μのタイヤ特性曲線の接線の傾きが同一となる結果を得ることができる。   FIG. 3 shows the relationship between tire characteristic curves of various road surfaces μ and arbitrary straight lines b, c, d passing through the origin of the tire characteristic curve. As shown in FIG. 3, as in FIG. 1, tangent slopes are obtained at intersections with arbitrary straight lines b, c, d for tire characteristic curves of various road surfaces μ. That is, for the tire characteristic curves on various road surfaces μ, tangent slopes are obtained at the intersections with the straight line b. For tire characteristic curves on various road surfaces μ, tangential slopes are obtained at intersections with the straight line c. With respect to tire characteristic curves on various road surfaces μ, tangent slopes are obtained at intersections with the straight line d. As a result, a result can be obtained in which the tangent slopes of the tire characteristic curves of various road surfaces μ obtained at the intersections with the same straight line are the same.

例えば、図4では、前記図3に示した直線cに着目している。図4に示すように、直線cとの交点での接線の傾きは各種路面μのタイヤ特性曲線で同一となる。すなわち、路面μがμ=0.2のタイヤ特性曲線との交点x1を示す制駆動力Fx1とスリップ率λ1との比(Fx1/λ1)を得る。また、路面μがμ=0.5のタイヤ特性曲線との交点x2を示す制駆動力Fx2とスリップ率λ2との比(Fx2/λ2)を得る。また、路面μがμ=1.0のタイヤ特性曲線との交点x3を示す制駆動力Fx3とスリップ率λ3との比(Fx3/λ3)を得る。そのようにして得た各値は同一値となる。そして、それら各交点x1,x2,x3での接線の傾きが同一値となる。   For example, FIG. 4 focuses on the straight line c shown in FIG. As shown in FIG. 4, the inclination of the tangent line at the intersection with the straight line c is the same in the tire characteristic curves of various road surfaces μ. That is, the ratio (Fx1 / λ1) between the braking / driving force Fx1 and the slip ratio λ1 indicating the intersection x1 with the tire characteristic curve with the road surface μ of μ = 0.2 is obtained. Further, a ratio (Fx2 / λ2) between the braking / driving force Fx2 and the slip ratio λ2 indicating the intersection x2 with the tire characteristic curve with the road surface μ of μ = 0.5 is obtained. Further, a ratio (Fx3 / λ3) between the braking / driving force Fx3 and the slip ratio λ3 indicating the intersection point x3 with the tire characteristic curve where the road surface μ is μ = 1.0 is obtained. Each value thus obtained is the same value. And the inclination of the tangent in each of these intersection x1, x2, x3 becomes the same value.

このように、路面μが異なっても、各タイヤ特性曲線について、制駆動力Fxとスリップ率λとの比(Fx/λ)が同一になる値(λ,Fx)で接線の傾きが同一となる。
そして、各タイヤ特性曲線で制駆動力Fxとスリップ率λとの比(Fx/λ)が同一となる値(λ,Fx)に関し、異なるタイヤ特性曲線間で得られる制駆動力Fx同士の比又はスリップ率λ同士の比は、路面μの比と等しくなる。
Thus, even if the road surface μ is different, the slope of the tangent line is the same for each tire characteristic curve at the value (λ, Fx) at which the ratio (Fx / λ) of the braking / driving force Fx and the slip ratio λ is the same. Become.
The ratio of the braking / driving force Fx obtained between the different tire characteristic curves with respect to the values (λ, Fx) at which the ratio (Fx / λ) of the braking / driving force Fx and the slip ratio λ is the same in each tire characteristic curve. Alternatively, the ratio between the slip ratios λ is equal to the ratio of the road surface μ.

図5を用いて、路面μが異なる各タイヤ特性曲線について、制駆動力Fx同士の比又はスリップ率λ同士の比と、その路面μの比との関係を説明する。図5には、路面μが異なる路面A(路面μ=μ)及び路面B(路面μ=μ)それぞれで得られるタイヤ特性曲線を示す。
図5に示すように、制駆動力Fxとスリップ率λとの比(Fx/λ)が同一となる値(λ,Fx)(同図中に■印、●印でそれぞれ示す値)でそれぞれ得られる制駆動力a2と制駆動力b2との比(a2/b2)と、路面Aの路面μ値μと路面Bの路面μ値μとの比(μ/μ)とは同一値になる。
The relationship between the ratio of braking / driving forces Fx or the ratio of slip ratios λ and the ratio of the road surface μ will be described with reference to FIG. 5 for each tire characteristic curve having a different road surface μ. FIG. 5 shows tire characteristic curves obtained respectively on the road surface A (road surface μ = μ A ) and the road surface B (road surface μ = μ B ) having different road surfaces μ.
As shown in FIG. 5, the ratio (Fx / λ) of the braking / driving force Fx and the slip ratio λ is the same (λ, Fx) (values indicated by ■ and ● in the same figure), respectively. What is the ratio (a2 / b2) between the braking / driving force a2 and the braking / driving force b2 and the ratio (μ A / μ B ) between the road surface μ value μ A of the road surface A and the road surface μ value μ B of the road surface B? It becomes the same value.

また、同じく、制駆動力Fxとスリップ率λとの比(Fx/λ)が同一となる値(λ,Fx)でそれぞれ得られるスリップ率a3とスリップ率b3との比(a3/b3)と、路面Aの路面μ値μと路面Bの路面μ値μとの比(μ/μ)とは同一値になる。
このようなことから、制駆動力Fxとスリップ率λとの比(Fx/λ)が同一となる値(λ,Fx)と原点(0,0)とをそれぞれ結んで得られる線長a1と線長b1との比(a1/b1)と、路面Aの路面μ値μと路面Bの路面μ値μとの比(μ/μ)とは同一値になる。このことは、幾何学的に次のように証明できる。
Similarly, the ratio (a3 / b3) of the slip ratio a3 and the slip ratio b3, which are respectively obtained with values (λ, Fx) at which the ratio (Fx / λ) of the braking / driving force Fx and the slip ratio λ is the same. becomes the same value as the ratio of the road surface mu values mu B of the road surface mu values mu a and the road surface B of road surface a (μ a / μ B) .
For this reason, the line length a1 obtained by connecting the value (λ, Fx) and the origin (0, 0) where the ratio (Fx / λ) of the braking / driving force Fx and the slip ratio λ is the same, and and the ratio of the line length b1 (a1 / b1), becomes the same value as the ratio of the road surface mu values mu B of the road surface mu values mu a and the road surface B of road surface a (μ a / μ B) . This can be proved geometrically as follows.

路面Aのタイヤ特性曲線を用いて描ける三角形(a1,a2,a3を辺とする三角形)と路面Bのタイヤ特性曲線を用いて描ける三角形(b1,b2,b3を辺とする三角形)とは相似の三角形となる。このことから、a1とb1との比と、a2とb2との比と、a3とb3との比とは、それぞれ同一値になる(a1:b1=a2:b2=a3:b3)。そして、制駆動力Fxについてのa2とb2との比(a2/b2)及びスリップ率λについてのa3とb3との比(a3/b3)は、路面Aの路面μ値μと路面Bの路面μ値μとの比(μ/μ)と同一値になる。よって、前述のように、線長a1と線長b1との比(a1/b1)と、路面Aの路面μ値μと路面Bの路面μ値μとの比(μ/μ)とは同一値となる結論を得ることができる。
以上のように制駆動力Fx同士の比、スリップ率λ同士の比又は前記線長同士の比を知ることができれば、路面μの比を知ることができる。
The triangle that can be drawn using the tire characteristic curve of road surface A (triangle with sides a1, a2, and a3) and the triangle that can be drawn using the tire characteristic curve of road surface B (triangle with sides b1, b2, and b3) are similar. It becomes a triangle. From this, the ratio of a1 and b1, the ratio of a2 and b2, and the ratio of a3 and b3 are the same value (a1: b1 = a2: b2 = a3: b3). And the ratio (a2 / b2) of a2 and b2 regarding the braking / driving force Fx and the ratio (a3 / b3) of a3 and b3 regarding the slip ratio λ are the values of the road surface μ μ value μ A and the road surface B. It becomes the same value as the ratio (μ A / μ B ) with the road surface μ value μ B. Therefore, as described above, the ratio between the line length a1 and the line length b1 (a1 / b1) and the ratio between the road surface μ value μ A of the road surface A and the road surface μ value μ B of the road surface B (μ A / μ B ) Can be concluded to be the same value.
As described above, if the ratio between the braking / driving forces Fx, the ratio between the slip ratios λ, or the ratio between the line lengths can be known, the ratio of the road surface μ can be known.

図6は、一例として、前記線長を基に走行路面の路面μを算出する演算手順を示す。ここでは、ある走行路面Bで得た制駆動力Fxb及びスリップ率λbを基に、既知の路面Aの路面μ値μのタイヤ特性曲線を参照して、ある走行路面Bの路面μ値μを算出する例を示す。
図6に示すように、先ずステップS1及びステップS2において、ある走行路面Bでの制駆動力Fxb及びスリップ率λbを検出する。続いてステップS3において、路面μ値μの路面Aのタイヤ特性曲線の原点(0,0)と実測点(λb,Fxb)とを通る直線が、そのタイヤ特性曲線と交わる点の値(λa,Fxa)を特定する。
FIG. 6 shows, as an example, a calculation procedure for calculating the road surface μ of the traveling road surface based on the line length. Here, based on the longitudinal force Fxb and slip ratio λb obtained in some road surface B, with reference to the tire characteristic curve of the road surface mu values mu A known road A, road mu values mu of a road surface B An example of calculating B will be shown.
As shown in FIG. 6, first, in step S1 and step S2, braking / driving force Fxb and slip ratio λb on a certain road surface B are detected. Next, in step S3 the origin (0, 0) and the measured point of the tire characteristic curve of the road surface A of road surface mu values mu A ([lambda] b, Fxb) and the straight line is the value of the point of intersection with the tire characteristic curve passing through ([lambda] a , Fxa).

続いてステップS4において、ある走行路面Bの路面μ値μの算出(推定)する。すなわち、前記実測点(λb,Fxb)と路面Aのタイヤ特性曲線の原点とを結ぶ直線の線長b1(=√(λb+Fxb))を得る。また、前記ステップS3で特定した路面Aのタイヤ特性曲線の交点の値(λa,Fxa)と該タイヤ特性曲線の原点とを結ぶ直線の線長a1(=√(λa+Fxa))を得る。さらに、線長b1と線長a1との比(b1/a1)を算出する。そして、その算出した比(b2/b1)と、路面Aの路面μ値μとを乗算し、その乗算値を走行路面Bの路面μ値μとして得る(μ=μ・b1/a1)。 Subsequently, in step S4, a road surface μ value μ B of a certain traveling road surface B is calculated (estimated). That is, a straight line length b1 (= √ (λb 2 + Fxb 2 )) connecting the actual measurement point (λb, Fxb) and the origin of the tire characteristic curve on the road surface A is obtained. Further, the straight line length a1 (= √ (λa 2 + Fxa 2 )) connecting the intersection value (λa, Fxa) of the tire characteristic curve on the road surface A specified in step S3 and the origin of the tire characteristic curve is obtained. . Further, the ratio (b1 / a1) between the line length b1 and the line length a1 is calculated. Then, its calculated ratio (b2 / b1), multiplying the road surface mu values mu A of road surface A, to obtain the multiplied value as the road surface mu value mu B of road surface B (μ B = μ A · b1 / a1).

図7は、路面μが異なる路面で得た制駆動力Fxとスリップ率λとの関係を示す。図7中、振動波形は、Dry路、Wet路及び低μ路で得た実測値を示す。また、点線は、それぞれの路面におけるタイヤ(ノーマルタイヤ)の特性曲線を示す。図7に示すように、路面μが異なる各路面におけるタイヤ特性曲線が、制駆動力Fxとスリップ率λとの比(Fx/λ)を維持しながらも、路面μが小さくなるほど制駆動力Fx及びスリップ率λが小さくなる。   FIG. 7 shows the relationship between the braking / driving force Fx and the slip ratio λ obtained on road surfaces having different road surfaces μ. In FIG. 7, the vibration waveform indicates actual values obtained on the Dry road, the Wet road, and the low μ road. A dotted line indicates a characteristic curve of a tire (normal tire) on each road surface. As shown in FIG. 7, the tire characteristic curve on each road surface with different road surface μ maintains the ratio (Fx / λ) between the braking / driving force Fx and the slip ratio λ, but the braking / driving force Fx decreases as the road surface μ decreases. And the slip ratio λ becomes small.

図8は、スタッドレスタイヤについて、路面μが異なる路面で得た制駆動力Fxとスリップ率λとの関係を示す。図8中、振動波形は、Dry路、Wet路及び低μ路で得た実測値を示す。また、点線は、それぞれの路面におけるタイヤ特性曲線を示す。また、太線の点線は、ノーマルタイヤのタイヤ特性曲線を示す。
図8に示すように、路面μが異なる各路面におけるタイヤ特性曲線(細線の点線)が、制駆動力Fxとスリップ率λとの比(Fx/λ)を維持しながらも、路面μが小さくなるほど、制駆動力Fx及びスリップ率λが小さくなる。さらに、ノーマルタイヤのタイヤ特性曲線(太線の点線)の制駆動力Fxとスリップ率λとの比(Fx/λ)と、スタッドレスタイヤのタイヤ特性曲線(細線の点線)の制駆動力Fxとスリップ率λとの比(Fx/λ)とが、同一値となっている。すなわち、ノーマルタイヤのタイヤ特性曲線とスタッドレスタイヤのタイヤ特性曲線とは相似形状となる。つまり、スタッドレスタイヤのようにグリップ力やタイヤの表面形状等が異なる場合でも、ノーマルタイヤのタイヤ特性曲線の制駆動力Fxとスリップ率λとの比(Fx/λ)と同一値となる。
FIG. 8 shows the relationship between the braking / driving force Fx and the slip ratio λ obtained on the road surfaces having different road surfaces μ for the studless tire. In FIG. 8, the vibration waveform indicates actual values obtained on the Dry road, the Wet road, and the low μ road. Moreover, a dotted line shows the tire characteristic curve in each road surface. A thick dotted line indicates a tire characteristic curve of a normal tire.
As shown in FIG. 8, the tire characteristic curve (thin dotted line) on each road surface with different road surface μ maintains the ratio (Fx / λ) of braking / driving force Fx and slip ratio λ, but the road surface μ is small. As it is, the braking / driving force Fx and the slip ratio λ are reduced. Furthermore, the ratio (Fx / λ) of the braking / driving force Fx and slip ratio λ of the tire characteristic curve (thick dotted line) of the normal tire, and the braking / driving force Fx and slip of the tire characteristic curve (thin dotted line) of the studless tire The ratio (Fx / λ) to the rate λ is the same value. That is, the tire characteristic curve of the normal tire and the tire characteristic curve of the studless tire have a similar shape. That is, even when the gripping force, the tire surface shape, and the like are different as in a studless tire, the ratio (Fx / λ) between the braking / driving force Fx and the slip ratio λ of the tire characteristic curve of the normal tire is the same value.

図9は、タイヤ特性曲線の任意点の制駆動力Fxとスリップ率λとの比(Fx/λ)と、その任意点でのタイヤ特性曲線の接線の傾き(∂制駆動力/∂スリップ率)との関係を示す。図9では、各路面μ(例えばμ=0.2、0.5、1.0)で得た値をプロットしている。図9に示すように、路面μにかかわらず、制駆動力Fxとスリップ率λとの比(Fx/λ)とタイヤ特性曲線の接線の傾きとが一定の関係を示している。   FIG. 9 shows the ratio (Fx / λ) between the braking / driving force Fx and the slip ratio λ at an arbitrary point of the tire characteristic curve and the slope of the tangent line of the tire characteristic curve at that arbitrary point (∂ braking / driving force / ∂ slip ratio). ). In FIG. 9, the values obtained for each road surface μ (for example, μ = 0.2, 0.5, 1.0) are plotted. As shown in FIG. 9, regardless of the road surface μ, the ratio of the braking / driving force Fx to the slip ratio λ (Fx / λ) and the slope of the tangent line of the tire characteristic curve show a constant relationship.

図10は、前記図9のプロット点を基に得た特性曲線を示す。図10に示すように、この特性曲線は、路面μにかかわらず、制駆動力Fxとスリップ率λとの比(Fx/λ)とタイヤ特性曲線の接線の傾きとが常に一定の関係があることを示すものとなる。
すなわち、乾燥アスファルト路面や凍結路面等、路面μが異なる路面であっても、この特性曲線は成立する。或いは、この特性曲線は、高摩擦係数を有する高摩擦路面用の高摩擦タイヤ特性曲線及び高摩擦係数より低い低摩擦係数を有する低摩擦路面用の低摩擦タイヤ特性曲線を含んでいると言える。このように図10に示す特性曲線は、図1と同様に、タイヤ特性曲線を示している。図1と区別して、図10の特性曲線を例えばグリップ特性曲線と呼ぶこともできる。
FIG. 10 shows a characteristic curve obtained based on the plotted points in FIG. As shown in FIG. 10, in this characteristic curve, the ratio (Fx / λ) between the braking / driving force Fx and the slip ratio λ and the slope of the tangent line of the tire characteristic curve are always constant regardless of the road surface μ. It will be shown.
That is, this characteristic curve is established even on a road surface having a different road surface μ, such as a dry asphalt road surface or a frozen road surface. Alternatively, it can be said that the characteristic curve includes a high friction tire characteristic curve for a high friction road surface having a high friction coefficient and a low friction tire characteristic curve for a low friction road surface having a low friction coefficient lower than the high friction coefficient. As described above, the characteristic curve shown in FIG. 10 is a tire characteristic curve as in FIG. Differentiating from FIG. 1, the characteristic curve of FIG. 10 can also be called a grip characteristic curve, for example.

この図10に示すように、制駆動力Fxとスリップ率λとの比(Fx/λ)が小さい領域(小レシオ領域)では、タイヤ特性曲線の接線の傾きが負値となる。そして、この領域では、その比(Fx/λ)が大きくなるに従い、タイヤ特性曲線の接線の傾きが一旦減少してから増加に転じる。ここで、タイヤ特性曲線の接線の傾きが負値であることは、制駆動力のスリップ率に関する偏微分係数が負値であることを示す。   As shown in FIG. 10, in the region where the ratio (Fx / λ) between the braking / driving force Fx and the slip ratio λ is small (small ratio region), the tangent slope of the tire characteristic curve has a negative value. In this region, as the ratio (Fx / λ) increases, the tangential slope of the tire characteristic curve once decreases and then increases. Here, the slope of the tangent line of the tire characteristic curve being a negative value indicates that the partial differential coefficient relating to the slip ratio of the braking / driving force is a negative value.

また、図10に示すように、制駆動力Fxとスリップ率λとの比(Fx/λ)が大きい領域(大レシオ領域)では、グリップ特性曲線の接線の傾きが正値になる。そして、この領域では、その比(Fx/λ)が大きくなると、タイヤ特性曲線の接線の傾きが増加する。すなわち、制駆動力Fxとスリップ率λとの比(Fx/λ)が大きい領域では、グリップ特性曲線は単調増加関数の形をしている。   Further, as shown in FIG. 10, in the region (large ratio region) where the ratio (Fx / λ) between the braking / driving force Fx and the slip ratio λ is large, the slope of the tangent line of the grip characteristic curve becomes a positive value. In this region, as the ratio (Fx / λ) increases, the tangential slope of the tire characteristic curve increases. That is, in the region where the ratio (Fx / λ) between the braking / driving force Fx and the slip ratio λ is large, the grip characteristic curve has a monotonically increasing function.

ここで、タイヤ特性曲線の接線の傾きが正値であることは、制駆動力のスリップ率に関する偏微分係数が正値であることを示す。また、タイヤ特性曲線の接線の傾きが最大であることは、該接線の傾きがタイヤ特性曲線の線形領域のものあることを示す。なお、線形領域では、タイヤ特性曲線の接線の傾きは、制駆動力Fxとスリップ率λとの比にかかわらず、常に一定の値を示す。   Here, the slope of the tangent line of the tire characteristic curve being a positive value indicates that the partial differential coefficient relating to the slip ratio of the braking / driving force is a positive value. In addition, the maximum inclination of the tangent line of the tire characteristic curve indicates that the inclination of the tangent line is in the linear region of the tire characteristic curve. In the linear region, the slope of the tangent line of the tire characteristic curve always shows a constant value regardless of the ratio between the braking / driving force Fx and the slip ratio λ.

このようにして得ることができるタイヤ特性曲線の接線の傾き(μ勾配、以下、Cp値ともいう。)は、グリップ特性パラメータ、タイヤのグリップ状態を表す変数又はタイヤが横方向に出せる力の飽和状態を表すパラメータとなる。
具体的には、タイヤ特性曲線の接線の傾きが正値の場合、スリップ率λを増やすことでさらに大きい制駆動力Fxを発生させることができることを示す。そして、タイヤ特性曲線の接線の傾きが零又は負値の場合、スリップ率λを増加させても制駆動力Fxが増えることはなく、逆に低下する恐れがあることを示す。
The slope of the tangent to the tire characteristic curve that can be obtained in this way (μ slope, hereinafter also referred to as Cp value) is a grip characteristic parameter, a variable that represents the grip state of the tire, or saturation of the force that the tire can exert in the lateral direction. It becomes a parameter indicating the state.
Specifically, when the slope of the tangent line of the tire characteristic curve is a positive value, it indicates that a larger braking / driving force Fx can be generated by increasing the slip ratio λ. When the slope of the tangent line of the tire characteristic curve is zero or a negative value, it indicates that the braking / driving force Fx does not increase even if the slip ratio λ is increased and may decrease.

このように、タイヤ特性曲線の接線の傾きからタイヤのグリップ力が限界領域であることを知ることができる。これにより、例えば、車輪のグリップ力が限界領域にあるときにも、タイヤのグリップ力の摩擦限界に対する余裕度を適切に推定できる。
なお、タイヤ特性曲線(図1)に対して偏微分計算を行い、連続的に描画することでグリップ特性曲線(図10)を得ることができる。
Thus, it can be known from the slope of the tangent to the tire characteristic curve that the grip force of the tire is in the limit region. Thereby, for example, even when the wheel grip force is in the limit region, it is possible to appropriately estimate the margin of the tire grip force with respect to the friction limit.
A grip characteristic curve (FIG. 10) can be obtained by performing partial differential calculation on the tire characteristic curve (FIG. 1) and drawing continuously.

本願発明者は、以上に述べたように、各路面μのタイヤ特性曲線について、そのタイヤ特性曲線の原点を通る任意の一の直線とタイヤ特性曲線との交点で、接線の傾きが同一となる点を発見した。すなわち、各路面μのタイヤ特性曲線について、制駆動力Fxとスリップ率λとの比(Fx/λ)が同一になる値(λ,Fx)で接線の傾きが同一となる点を発見した。   As described above, the inventor of the present application has the same tangential slope at the intersection of any one straight line passing through the origin of the tire characteristic curve and the tire characteristic curve for the tire characteristic curve of each road surface μ. I found a spot. That is, with respect to the tire characteristic curve of each road surface μ, a point was found where the slope of the tangent line was the same at the value (λ, Fx) where the ratio (Fx / λ) of the braking / driving force Fx and the slip ratio λ was the same.

これにより、本願発明者は、路面μにかかわらず、制駆動力Fxとスリップ率λとの比(Fx/λ)とタイヤ特性曲線の接線の傾きとの関係がある特性曲線(グリップ特性曲線)として表せる結果を得た(図10)。この結果を利用することで、制駆動力Fxとスリップ率λとがわかれば、特性曲線(グリップ特性曲線)を基に、路面μの情報を必要とすることなく、タイヤの摩擦状態の情報を得ることができる。   Thereby, the inventor of the present application has a characteristic curve (grip characteristic curve) having a relationship between the ratio of the braking / driving force Fx and the slip ratio λ (Fx / λ) and the slope of the tangent line of the tire characteristic curve regardless of the road surface μ. The result which can be expressed as was obtained (FIG. 10). By using this result, if the braking / driving force Fx and the slip ratio λ are known, based on the characteristic curve (grip characteristic curve), the information on the frictional state of the tire can be obtained without requiring information on the road surface μ. Obtainable.

また、本願発明者は、路面μが異なるタイヤ特性曲線で、制駆動力Fxとスリップ率λとの比(Fx/λ)が同一となる値(λ,Fx)での制駆動力Fx同士の比、スリップ率λ同士の比又は前記線長同士の比が、路面μの比と等しくなる点を発見した。
これにより、制駆動力Fx同士の比、スリップ率λ同士の比、又は線長同士の比がわかれば、路面μの比を知ることができる。
Further, the inventor of the present application uses a tire characteristic curve with different road surface μ, and the braking / driving forces Fx between the braking / driving forces Fx at values (λ, Fx) at which the ratio (Fx / λ) of the braking / driving force Fx and the slip ratio λ is the same. It has been found that the ratio, the ratio between the slip ratios λ or the ratio between the line lengths becomes equal to the ratio of the road surface μ.
Thereby, if the ratio between the braking / driving forces Fx, the ratio between the slip ratios λ, or the ratio between the line lengths is known, the ratio of the road surface μ can be known.

(2)車輪のスリップ角と車輪の横力との関係
図11はタイヤ特性曲線を示す。このタイヤ特性曲線は、車輪のスリップ角βtと車輪の横力Fyとの間に成立する一般的な相関関係を示す。例えば、タイヤモデルを実験データを基にチューニングすることで、前後輪それぞれで二輪分の等価特性図(タイヤ特性曲線)を得る。ここで、例えば、マジックフォーミュラ(MagicFormula)を基にタイヤモデルを構築している。横力Fyは、コーナリングフォースやサイドフォースに代表される値である。ここで、横力Fyは、タイヤから地面に作用する力である。また、横力Fyが接地面において車輪に作用する車輪力に相当する。車輪のスリップ角βtが車輪のスリップ度に相当する。
(2) Relationship between wheel slip angle and wheel lateral force FIG. 11 shows a tire characteristic curve. This tire characteristic curve shows a general correlation established between the wheel slip angle βt and the wheel lateral force Fy. For example, by tuning a tire model based on experimental data, an equivalent characteristic diagram (tire characteristic curve) for two wheels is obtained for each of the front and rear wheels. Here, for example, a tire model is constructed on the basis of a magic formula. The lateral force Fy is a value represented by a cornering force or a side force. Here, the lateral force Fy is a force acting on the ground from the tire. Further, the lateral force Fy corresponds to the wheel force acting on the wheel on the ground contact surface. The wheel slip angle βt corresponds to the slip degree of the wheel.

図11に示すように、タイヤ特性曲線では、スリップ角βtと横力Fyとの関係が、スリップ角βtの絶対値が増加するに従い線形から非線形に遷移する。すなわち、タイヤ特性曲線では、スリップ角βtが零から所定の範囲内にある場合には、スリップ角βtと横力Fyとの間に線形関係が成り立つ。そして、タイヤ特性曲線では、スリップ角βt(絶対値)がある程度大きくなると(前記所定の範囲を超えると)、スリップ角βtと横力Fyとの関係が非線形関係になる。このように、タイヤ特性曲線は、線形部分と非線形部分とを有する。   As shown in FIG. 11, in the tire characteristic curve, the relationship between the slip angle βt and the lateral force Fy changes from linear to non-linear as the absolute value of the slip angle βt increases. That is, in the tire characteristic curve, when the slip angle βt is within a predetermined range from zero, a linear relationship is established between the slip angle βt and the lateral force Fy. In the tire characteristic curve, when the slip angle βt (absolute value) increases to some extent (exceeding the predetermined range), the relationship between the slip angle βt and the lateral force Fy becomes a non-linear relationship. Thus, the tire characteristic curve has a linear portion and a non-linear portion.

このようなスリップ角βtと横力Fyとの間にある関係や線形関係から非線形関係への遷移は、タイヤ特性曲線の接線の傾き(勾配)に着目すれば一目瞭然である。ここでいうタイヤ特性曲線の接線の傾きとは、スリップ角βtの変化量と横力Fyの変化量との比、すなわち、横力Fyのスリップ角βtに関する偏微分係数で示される値である。
ここで、図11に示すように、タイヤ特性曲線の原点を通る任意の直線a,b,c,…を描く。すると、タイヤ特性曲線に対して交わる任意の直線a,b,c,…との交点(図11中に○印で示す交点)でタイヤ特性曲線の接線の傾きを得ることができる。そして、タイヤ特性曲線の接線の傾きは各交点で異なるものとなる。このようなタイヤ特性曲線の接線の傾きに着目することで、スリップ角βtと横力Fyとの間にある関係や線形関係から非線形関係への遷移の状態を知ることができる。
The transition from the relationship between the slip angle βt and the lateral force Fy or the linear relationship to the non-linear relationship is obvious when attention is paid to the slope (gradient) of the tangent line of the tire characteristic curve. The inclination of the tangent line of the tire characteristic curve here is a value represented by a ratio of a change amount of the slip angle βt and a change amount of the lateral force Fy, that is, a partial differential coefficient related to the slip angle βt of the lateral force Fy.
Here, as shown in FIG. 11, arbitrary straight lines a, b, c,... Passing through the origin of the tire characteristic curve are drawn. Then, the tangent slope of the tire characteristic curve can be obtained at the intersections (intersections indicated by circles in FIG. 11) with arbitrary straight lines a, b, c,... Intersecting the tire characteristic curve. The slope of the tangent line of the tire characteristic curve is different at each intersection. By paying attention to the inclination of the tangent line of the tire characteristic curve, it is possible to know the relationship between the slip angle βt and the lateral force Fy or the state of transition from the linear relationship to the non-linear relationship.

これにより、タイヤの摩擦状態の推定も可能になる。例えば、図11に示すように、タイヤ特性曲線上で、非線形域でも線形域に近い位置x0にあれば、タイヤの摩擦状態が安定状態にあると推定できる。そして、タイヤの摩擦状態が安定状態であれば、例えばタイヤがその能力を発揮できるレベルにあると推定できる。又は車両が安定状態にあると推定できる。   Thereby, estimation of the friction state of the tire is also possible. For example, as shown in FIG. 11, if the tire characteristic curve is at a position x0 that is close to the linear region even in the nonlinear region, it can be estimated that the tire friction state is in a stable state. And if the friction state of a tire is a stable state, it can be estimated that a tire is in the level which can exhibit the capability, for example. Alternatively, it can be estimated that the vehicle is in a stable state.

図12は、各種路面μのタイヤ特性曲線と摩擦円を示す。図12(a)は、各種路面μのタイヤ特性曲線を示す。図12(b)〜(d)は、各路面μの摩擦円を示す。路面μは例えば0.2、0.5、1.0である。図12(a)に示すように、タイヤ特性曲線は、各路面μで定性的に同様な傾向を示す。また、図12(b)〜(d)に示すように、路面μが小さくなるほど摩擦円が小さくなる。すなわち、路面μが小さくなるほどタイヤが許容できる横力が小さくなる。このように、タイヤ特性は、路面摩擦係数(路面μ)をパラメータとした特性となる。よって、図12に示すように、路面摩擦係数の値に応じて、低摩擦の場合のタイヤ特性曲線、中摩擦の場合のタイヤ特性曲線、及び高摩擦の場合のタイヤ特性曲線等を得ることができる。   FIG. 12 shows tire characteristic curves and friction circles of various road surfaces μ. FIG. 12A shows tire characteristic curves of various road surfaces μ. 12 (b) to 12 (d) show the friction circle of each road surface μ. The road surface μ is, for example, 0.2, 0.5, or 1.0. As shown in FIG. 12 (a), the tire characteristic curve shows the same tendency qualitatively at each road surface μ. Further, as shown in FIGS. 12B to 12D, the friction circle becomes smaller as the road surface μ becomes smaller. That is, as the road surface μ decreases, the lateral force that the tire can tolerate decreases. As described above, the tire characteristics are characteristics using the road surface friction coefficient (road surface μ) as a parameter. Therefore, as shown in FIG. 12, a tire characteristic curve in the case of low friction, a tire characteristic curve in the case of medium friction, a tire characteristic curve in the case of high friction, and the like can be obtained according to the value of the road surface friction coefficient. it can.

図13は、各種路面μのタイヤ特性曲線と原点を通る任意の直線a,b,cとの関係を示す。図13に示すように、前記図11と同様に、各種路面μのタイヤ特性曲線について、任意の直線a,b,cとの交点で接線の傾きを得る。すなわち、各種路面μでのタイヤ特性曲線について、直線aとの交点で接線の傾きをそれぞれ得る。各種路面μでのタイヤ特性曲線について、直線bとの交点で接線の傾きをそれぞれ得る。各種路面μでのタイヤ特性曲線について、直線cとの交点で接線の傾きをそれぞれ得る。その結果、同一直線との交点で得られる各種路面μのタイヤ特性曲線の接線の傾きが同一となる結果を得ることができる。   FIG. 13 shows the relationship between tire characteristic curves of various road surfaces μ and arbitrary straight lines a, b, c passing through the origin. As shown in FIG. 13, as in FIG. 11, tangent slopes are obtained at intersections with arbitrary straight lines a, b, c for tire characteristic curves of various road surfaces μ. That is, for the tire characteristic curves on various road surfaces μ, tangent slopes are obtained at the intersections with the straight line a. For tire characteristic curves on various road surfaces μ, tangent slopes are obtained at intersections with the straight line b. For tire characteristic curves on various road surfaces μ, tangential slopes are obtained at intersections with the straight line c. As a result, a result can be obtained in which the tangent slopes of the tire characteristic curves of various road surfaces μ obtained at the intersections with the same straight line are the same.

例えば、図14では、前記図13に示した直線cに着目している。図14に示すように、直線cとの交点での接線の傾きは各種路面μのタイヤ特性曲線で同一となる。すなわち、路面μがμ=0.2のタイヤ特性曲線との交点x1を示す横力Fy1とスリップ角βt1との比(Fy1/βt1)を得る。また、路面μがμ=0.5のタイヤ特性曲線との交点x2を示す横力Fy2とスリップ角βt2との比(Fy2/βt2)を得る。また、路面μがμ=1.0のタイヤ特性曲線との交点x3を示す横力Fy3とスリップ角βt3との比(Fy3/βt3)を得る。そのようにして得た各値は同一値となる。そして、各交点x1,x2,x3での接線の傾きが同一値となる。   For example, in FIG. 14, attention is paid to the straight line c shown in FIG. As shown in FIG. 14, the inclination of the tangent line at the intersection with the straight line c is the same in the tire characteristic curves of various road surfaces μ. That is, the ratio (Fy1 / βt1) between the lateral force Fy1 and the slip angle βt1 indicating the intersection x1 with the tire characteristic curve with the road surface μ of μ = 0.2 is obtained. Further, a ratio (Fy2 / βt2) between the lateral force Fy2 and the slip angle βt2 indicating the intersection x2 with the tire characteristic curve with the road surface μ of μ = 0.5 is obtained. Further, a ratio (Fy3 / βt3) between the lateral force Fy3 and the slip angle βt3 indicating the intersection x3 with the tire characteristic curve with the road surface μ of μ = 1.0 is obtained. Each value thus obtained is the same value. And the inclination of the tangent line in each intersection x1, x2, x3 becomes the same value.

このように、路面μが異なっても、各タイヤ特性曲線について、横力Fyとスリップ角βtとの比(Fy/βt)が同一になる値(βt,Fy)において接線の傾きが同一となる。
そして、各タイヤ特性曲線で横力Fyとスリップ角βtとの比(Fy/βt)が同一となる値(βt,Fy)に関し、異なるタイヤ特性曲線で得られる横力Fy同士の比又はスリップ角βt同士の比は、路面μの比と等しくなる。
Thus, even if the road surface μ is different, the slope of the tangent line is the same for each tire characteristic curve at the value (βt, Fy) where the ratio (Fy / βt) between the lateral force Fy and the slip angle βt is the same. .
Then, regarding the values (βt, Fy) at which the ratio (Fy / βt) between the lateral force Fy and the slip angle βt is the same in each tire characteristic curve, the ratio or slip angle between the lateral forces Fy obtained with different tire characteristic curves. The ratio between βt is equal to the ratio of the road surface μ.

図15を用いて、路面μが異なる各タイヤ特性曲線について、横力Fy同士の比又はスリップ角βt同士の比と、その路面μの比との関係を説明する。図15には、路面μが異なる路面A(路面μ=μ)及び路面B(路面μ=μ)それぞれで得られるタイヤ特性曲線を示す。
図15に示すように、横力Fyとスリップ角βtとの比(Fy/βt)が同一となる値(βt,Fy)(同図中に■印、●印でそれぞれ示す値)でそれぞれ得られる横力a2と横力b2との比(a2/b2)と、路面Aの路面μ値μと路面Bの路面μ値μとの比(μ/μ)とは同一値になる。
The relationship between the ratio of the lateral forces Fy or the ratio of the slip angles βt and the ratio of the road surface μ will be described with reference to FIG. 15 for each tire characteristic curve having a different road surface μ. FIG. 15 shows tire characteristic curves obtained on the road surface A (road surface μ = μ A ) and the road surface B (road surface μ = μ B ) having different road surfaces μ.
As shown in FIG. 15, the values (βt, Fy) in which the ratio (Fy / βt) between the lateral force Fy and the slip angle βt are the same (values indicated by ■ and ● in the same figure), respectively. The ratio of the lateral force a2 and the lateral force b2 (a2 / b2) and the ratio (μ A / μ B ) between the road surface μ value μ A of the road surface A and the road surface μ value μ B of the road surface B are the same value. Become.

また、同じく、横力Fyとスリップ角βtとの比(Fy/βt)が同一となる値(βt,Fy)でそれぞれ得られるスリップ率a3とスリップ率b3との比(a3/b3)と、路面Aの路面μ値μと路面Bの路面μ値μとの比(μ/μ)とは同一値になる。
このようなことから、路面Aで得られるタイヤ特性曲線と路面Bで得られるタイヤ特性曲線とで、横力Fyとスリップ角βtとの比(Fy/βt)が同一となる値(βt,Fy)と原点(0,0)とをそれぞれ結んで得られる線長a1と線長b1との比(a1/b1)と、路面Aの路面μ値μと路面Bの路面μ値μとの比(μ/μ)とは同一値になる。このことは、幾何学的に次のように証明できる。
Similarly, the ratio (a3 / b3) between the slip ratio a3 and the slip ratio b3, which are respectively obtained with values (βt, Fy) at which the ratio (Fy / βt) between the lateral force Fy and the slip angle βt is the same, The ratio (μ A / μ B ) between the road surface μ value μ A of the road surface A and the road surface μ value μ B of the road surface B is the same value.
Therefore, the tire characteristic curve obtained on the road surface A and the tire characteristic curve obtained on the road surface B have the same ratio (Fy / βt) between the lateral force Fy and the slip angle βt (βt, Fy). ) And the origin (0, 0), respectively, the ratio (a1 / b1) of the line length a1 and the line length b1, and the road surface μ value μ A of the road surface A and the road surface μ value μ B of the road surface B It becomes the same value as the ratio (μ a / μ B) of. This can be proved geometrically as follows.

路面Aのタイヤ特性曲線を用いて得られる三角形(a1,a2,a3を辺とする三角形)と路面Bのタイヤ特性曲線を用いて得られる三角形(b1,b2,b3を辺とする三角形)とは相似の三角形となる。このことから、a1とb1との比と、a2とb2との比と、a3とb3との比とは、それぞれ同一値になる(a1:b1=a2:b2=a3:b3)。そして、横力Fyについてのa2とb2との比及びスリップ角βtについてのa3とb3との比は、路面Aの路面μ値μと路面Bの路面μ値μとの比(μ/μ)と同一値になる。よって、前述のように、線長a1と線長b1との比(a1/b1)と、路面Aの路面μ値μと路面Bの路面μ値μとの比(μ/μ)とは同一値となる結論を得ることができる。 A triangle (triangle with sides a1, a2 and a3) obtained using the tire characteristic curve of road surface A and a triangle (triangle with sides b1, b2 and b3) obtained using the tire characteristic curve of road surface B, and Becomes a similar triangle. From this, the ratio of a1 and b1, the ratio of a2 and b2, and the ratio of a3 and b3 are the same value (a1: b1 = a2: b2 = a3: b3). The ratio of a2 and b2 for the lateral force Fy and the ratio of a3 and b3 for the slip angle βt are the ratio of the road surface μ value μ A of the road surface A and the road surface μ value μ B of the road surface B (μ A / Μ B ). Therefore, as described above, the ratio between the line length a1 and the line length b1 (a1 / b1) and the ratio between the road surface μ value μ A of the road surface A and the road surface μ value μ B of the road surface B (μ A / μ B ) Can be concluded to be the same value.

図16は、一例として、前記線長を基に走行路面の路面μを算出する演算手順を示す。ここでは、ある走行路面Bで得た横力Fyb及びスリップ角βtbを基に、既知の路面Aの路面μ値μのタイヤ特性曲線を参照して、ある走行路面Bの路面μ値μを算出する例を示す。
図16に示すように、先ずステップS11及びステップS12において、ある走行路面Bでの横力Fyb及びスリップ角βtbを検出する。続いてステップS13において、路面μ値μの路面Aのタイヤ特性曲線の原点(0,0)と実測点(βtb,Fyb)とを通る直線が、そのタイヤ特性曲線と交わる点の値(βta,Fya)を特定する。
FIG. 16 shows, as an example, a calculation procedure for calculating the road surface μ of the traveling road surface based on the line length. Here, based on the lateral force Fyb and the slip angle βtb obtained on a certain road surface B, a road surface μ value μ B of a certain road surface B is referred to with reference to a known tire characteristic curve of the road surface μ value μ A of the road surface A. An example of calculating is shown.
As shown in FIG. 16, first, in step S11 and step S12, the lateral force Fyb and the slip angle βtb on a certain road surface B are detected. Then In step S13, the origin (0, 0) and the measured point of the tire characteristic curve of the road surface A of road surface mu values μ A (βtb, Fyb) and the straight line is the value of the point of intersection with the tire characteristic curve passing through (Betata , Fya).

続いてステップS14において、ある走行路面Bの路面μ値μの算出(推定)する。すなわち、前記実測点(βtb,Fyb)と路面Aのタイヤ特性曲線の原点とを結ぶ直線の線長b1(=√(βtb+Fyb))を得る。また、前記ステップS13で特定した路面Aのタイヤ特性曲線の交点の値(βta,Fya)と該タイヤ特性曲線の原点とを結ぶ直線の線長a1(=√(βta+Fya))を得る。さらに、線長b1と線長a1との比(b1/a1)を算出する。そして、その算出した比(b2/b1)と、路面Aの路面μ値μとを乗算し、その乗算値を走行路面Bの路面μ値μとして得る(μ=μ・b1/a1)。 Subsequently, in step S14, a road surface μ value μ B of a certain traveling road surface B is calculated (estimated). That is, a straight line length b1 (= √ (βtb 2 + Fyb 2 )) connecting the actual measurement point (βtb, Fyb) and the origin of the tire characteristic curve on the road surface A is obtained. Further, a straight line length a1 (= √ (βta 2 + Fya 2 )) connecting the intersection value (βta, Fya) of the tire characteristic curve on the road surface A specified in step S13 and the origin of the tire characteristic curve is obtained. . Further, the ratio (b1 / a1) between the line length b1 and the line length a1 is calculated. Then, its calculated ratio (b2 / b1), multiplying the road surface mu values mu A of road surface A, to obtain the multiplied value as the road surface mu value mu B of road surface B (μ B = μ A · b1 / a1).

図17は、横軸にスリップ度Sをとり、縦軸にタイヤ力Fをとっている。
ここで、制駆動力Fx及び横力Fyは、それら値を含む概念のタイヤ力(車輪力)Fとして観念でき、スリップ率λ及びスリップ角βtは、それら値を含む概念のスリップ度Sとして観念できる。また、例えば、制駆動力Fxと横力Fyとの合力も、タイヤ力Fとして観念できる。
In FIG. 17, the horizontal axis represents the slip degree S, and the vertical axis represents the tire force F.
Here, the braking / driving force Fx and the lateral force Fy can be considered as a conceptual tire force (wheel force) F including these values, and the slip ratio λ and the slip angle βt are conceptualized as a slip degree S of the concept including these values. it can. Further, for example, the resultant force of the braking / driving force Fx and the lateral force Fy can be considered as the tire force F.

このように制駆動力Fx及び横力Fyがタイヤ力Fとして観念でき、スリップ率λ及びスリップ角βtがスリップ度Sとして観念できることから、タイヤ力F及びスリップ度Sについても、前記図5や図15に示したような関係を得ることができる。
よって、図17に示すように、路面μが異なる各タイヤ特性曲線について、タイヤ力F同士の比(a2/b2)、スリップ度S同士の比(a3/b3)又は線長の比(a1/b1)と、その路面μの比(μ/μ)とが等しくなる。
Thus, since the braking / driving force Fx and the lateral force Fy can be considered as the tire force F, and the slip ratio λ and the slip angle βt can be considered as the slip degree S, the tire force F and the slip degree S are also shown in FIGS. The relationship as shown in FIG. 15 can be obtained.
Therefore, as shown in FIG. 17, for each tire characteristic curve having a different road surface μ, the ratio of tire forces F (a2 / b2), the ratio of slip degrees S (a3 / b3), or the ratio of line lengths (a1 / and b1), the ratio of the road surface μ (μ a / μ B) and are equal.

図18は、タイヤ特性曲線の任意点の横力Fyとスリップ角βtとの比(Fy/βt)と、その任意点でのタイヤ特性曲線の接線の傾き(∂Fy/∂βt)との関係を示す。図18に示すように、どの各路面μ(例えばμ=0.2、0.5、1.0)でも、横力Fyとスリップ角βtとの比(Fy/βt)とタイヤ特性曲線の接線の傾きとが一定の関係を示している。   FIG. 18 shows the relationship between the ratio (Fy / βt) between the lateral force Fy and the slip angle βt at an arbitrary point of the tire characteristic curve and the tangential slope (∂Fy / ∂βt) of the tire characteristic curve at the arbitrary point. Indicates. As shown in FIG. 18, the ratio (Fy / βt) between the lateral force Fy and the slip angle βt and the tangent line of the tire characteristic curve at any road surface μ (for example, μ = 0.2, 0.5, 1.0). Shows a certain relationship with the slope.

すなわち、乾燥アスファルト路面や凍結路面等、路面μが異なる路面であっても、この特性曲線は成立する。或いは、この特性曲線は、高摩擦係数を有する高摩擦路面用の高摩擦タイヤ特性曲線及び高摩擦係数より低い低摩擦係数を有する低摩擦路面用の低摩擦タイヤ特性曲線を含んでいると言える。ここで、このように図18に示す特性曲線は、図11と同様に、タイヤ特性曲線を示している。図11と区別して、図18の特性曲線を例えばグリップ特性曲線と呼ぶこともできる。   That is, this characteristic curve is established even on a road surface having a different road surface μ, such as a dry asphalt road surface or a frozen road surface. Alternatively, it can be said that the characteristic curve includes a high friction tire characteristic curve for a high friction road surface having a high friction coefficient and a low friction tire characteristic curve for a low friction road surface having a low friction coefficient lower than the high friction coefficient. Here, the characteristic curve shown in FIG. 18 is a tire characteristic curve like FIG. Differentiating from FIG. 11, the characteristic curve of FIG. 18 can also be called a grip characteristic curve, for example.

この図18に示すように、横力Fyとスリップ角βtとの比(Fy/βt)が小さい領域(小レシオ領域)では、タイヤ特性曲線の接線の傾きが負値となる。そして、この領域では、その比(Fy/βt)が大きくなるに従い、タイヤ特性曲線の接線の傾きが一旦減少してから増加に転じる。ここで、タイヤ特性曲線の接線の傾きが負値であることは、横力のスリップ角に関する偏微分係数が負値であることを示す。   As shown in FIG. 18, in the region where the ratio (Fy / βt) between the lateral force Fy and the slip angle βt is small (small ratio region), the tangent slope of the tire characteristic curve becomes a negative value. In this region, as the ratio (Fy / βt) increases, the tangential slope of the tire characteristic curve once decreases and then increases. Here, the negative slope of the tangent of the tire characteristic curve indicates that the partial differential coefficient regarding the slip angle of the lateral force is a negative value.

また、図18に示すように、横力Fyとスリップ角βtとの比(Fy/βt)が大きい領域(大レシオ領域)では、タイヤ特性曲線の接線の傾きが正値になる。そして、この領域では、その比(Fy/βt)が大きくなると、タイヤ特性曲線の接線の傾きが増加する。すなわち、横力Fyとスリップ角βtとの比(Fy/βt)が大きい領域では、グリップ特性曲線は単調増加関数の形をしている。   Further, as shown in FIG. 18, in the region where the ratio (Fy / βt) between the lateral force Fy and the slip angle βt is large (large ratio region), the tangent slope of the tire characteristic curve becomes a positive value. In this region, as the ratio (Fy / βt) increases, the tangential slope of the tire characteristic curve increases. That is, in the region where the ratio (Fy / βt) between the lateral force Fy and the slip angle βt is large, the grip characteristic curve has a monotonically increasing function.

ここで、タイヤ特性曲線の接線の傾きが正値であることは、横力のスリップ角に関する偏微分係数が正値であることを示す。また、タイヤ特性曲線の接線の傾きが最大であることは、該接線の傾きがタイヤ特性曲線の線形領域のものであることを示す。なお、線形領域では、タイヤ特性曲線の接線の傾きは、横力Fyとスリップ角βtとの比にかかわらず、常に一定の値を示す。   Here, the inclination of the tangent line of the tire characteristic curve being a positive value indicates that the partial differential coefficient regarding the slip angle of the lateral force is a positive value. In addition, the maximum inclination of the tangent line of the tire characteristic curve indicates that the inclination of the tangent line is in the linear region of the tire characteristic curve. In the linear region, the slope of the tangent line of the tire characteristic curve always shows a constant value regardless of the ratio between the lateral force Fy and the slip angle βt.

このようにして得ることができるタイヤ特性曲線の接線の傾き(μ勾配)は、グリップ特性パラメータ、タイヤのグリップ状態を表す変数又はタイヤが横方向に出せる力の飽和状態を表すパラメータとなる。具体的には、タイヤ特性曲線の接線の傾きが正値の場合、スリップ角βtを増やすことでさらに強い横力Fy(コーナリングフォース等)を発生させることができることを示す。そして、タイヤ特性曲線の接線の傾きが零又は負値の場合、スリップ角βtを増加させても横力Fy(コーナリングフォース等)が増えることはなく、逆に低下する恐れがあることを示す。このように、タイヤ特性曲線の接線の傾きからタイヤのグリップ力が限界領域であることを知ることができる。これにより、例えば、車輪のグリップ力が限界領域にあるときにも、タイヤのグリップ力の摩擦限界に対する余裕度を適切に推定できる。   The tangential slope (μ slope) of the tire characteristic curve that can be obtained in this way is a grip characteristic parameter, a variable that represents the grip state of the tire, or a parameter that represents a saturated state of force that the tire can exert in the lateral direction. Specifically, when the slope of the tangent line of the tire characteristic curve is a positive value, it indicates that a stronger lateral force Fy (cornering force or the like) can be generated by increasing the slip angle βt. If the slope of the tangent line of the tire characteristic curve is zero or a negative value, it indicates that even if the slip angle βt is increased, the lateral force Fy (cornering force or the like) does not increase and may decrease. Thus, it can be known from the slope of the tangent to the tire characteristic curve that the grip force of the tire is in the limit region. Thereby, for example, even when the wheel grip force is in the limit region, it is possible to appropriately estimate the margin of the tire grip force with respect to the friction limit.

なお、タイヤ特性曲線(図11)に対して偏微分計算を行い、連続的に描画することでグリップ特性曲線(図18)を得ることができる。
本願発明者は、以上に述べたように、各路面μのタイヤ特性曲線について、そのタイヤ特性曲線の原点を通る任意の一の直線とタイヤ特性曲線との交点で、接線の傾きが同一となる点を発見した。すなわち、各路面μのタイヤ特性曲線について、横力Fyとスリップ角βtとの比(Fy/βt)が同一になる値(βt,Fy)で接線の傾きが同一となる点を発見した。
A grip characteristic curve (FIG. 18) can be obtained by performing partial differential calculation on the tire characteristic curve (FIG. 11) and drawing continuously.
As described above, the inventor of the present application has the same tangential slope at the intersection of any one straight line passing through the origin of the tire characteristic curve and the tire characteristic curve for the tire characteristic curve of each road surface μ. I found a spot. That is, the tire characteristic curve of each road surface μ was found to have the same tangent slope at a value (βt, Fy) at which the ratio (Fy / βt) of the lateral force Fy to the slip angle βt is the same.

これにより、本願発明者は、路面μにかかわらず、横力Fyとスリップ角βtとの比(Fy/βt)とタイヤ特性曲線の接線の傾きとの関係がある特性曲線(グリップ特性曲線)として表せる結果を得た(図18)。この結果を利用することで、横力Fyとスリップ角βtとがわかれば、特性曲線(グリップ特性曲線)を基に、路面μの情報を必要とすることなく、タイヤの摩擦状態の情報を得ることができる。   Accordingly, the inventor of the present application uses a characteristic curve (grip characteristic curve) having a relationship between the ratio of the lateral force Fy and the slip angle βt (Fy / βt) and the slope of the tangent line of the tire characteristic curve regardless of the road surface μ. The result which can be expressed was obtained (FIG. 18). By using this result, if the lateral force Fy and the slip angle βt are known, information on the friction state of the tire is obtained based on the characteristic curve (grip characteristic curve) without requiring information on the road surface μ. be able to.

また、本願発明者は、路面μが異なるタイヤ特性曲線で、横力Fyとスリップ角βtとの比(Fy/βt)が同一となる値(βt,Fy)での横力Fy同士の比、スリップ角βt同士の比、又は前記線長同士の比が、路面μの比と等しくなる点を発見した。
これにより、横力Fy同士の比、スリップ角βt同士の比、又は線長同士の比がわかれば、路面μの比を知ることができる。
Further, the inventor of the present application is a tire characteristic curve with different road surface μ, and the ratio between the lateral forces Fy at the values (βt, Fy) where the ratio (Fy / βt) between the lateral force Fy and the slip angle βt is the same, It has been found that the ratio between the slip angles βt or the ratio between the line lengths becomes equal to the ratio of the road surface μ.
Thereby, if the ratio between the lateral forces Fy, the ratio between the slip angles βt, or the ratio between the line lengths is known, the ratio of the road surface μ can be known.

(3)タイヤ摩擦円と車輪の車輪力(タイヤ力)との関係
図19は、前後方向のグリップ力に基づく制駆動力FxをX軸、横方向のグリップ力に基づく横力FyをY軸上で表現する直交座標面上にタイヤ摩擦円を表現したものである。
ここで、タイヤ摩擦円は、タイヤが接地面において摩擦状態を維持できる摩擦限界を示す。
すなわち、タイヤ摩擦円に対して、制駆動動力Fxや横力Fy、又は制駆動動力Fxと横力Fyとの合力の値が、タイヤ摩擦円の内側にある場合、摩擦限界に達しておらず摩擦状態を保っている状態を示す。
(3) Relationship between the tire friction circle and the wheel force (tire force) of the wheel FIG. 19 shows the braking / driving force Fx based on the longitudinal grip force as the X axis and the lateral force Fy based on the lateral grip force as the Y axis. The tire friction circle is expressed on the orthogonal coordinate plane expressed above.
Here, the tire friction circle indicates a friction limit at which the tire can maintain a friction state on the contact surface.
That is, if the value of the resultant force of the braking / driving power Fx, the lateral force Fy, or the braking / driving power Fx and the lateral force Fy is within the tire friction circle, the friction limit is not reached. The state where the friction state is maintained is shown.

また、その値がタイヤ摩擦円と一致した場合、最大の摩擦力を発揮している状態を示す。すなわち、タイヤと接地面との間の摩擦力の最大値によってタイヤ摩擦円の大きさが決まる。つまり、制駆動動力Fxと横力Fyとの合力の最大値を、そのときの合力の方向に合わせてプロットしていくことで、楕円形状のタイヤ摩擦円を描くことができる。
また、タイヤ接地面においてタイヤに加わる外力が、タイヤ摩擦円よりも大きい場合、タイヤが接地面との間で摩擦状態を保っていない状態、つまり、タイヤと地面との相対変位が大きくなり、いわゆるスリップ状態であることを示す。これは、タイヤ摩擦円と前後方向及び横方向のグリップ力との関係が、前後方向と横方向とにそれぞれ同時に最大グリップ力を発揮することができないことを意味する。
Moreover, when the value corresponds with a tire friction circle, the state which is exhibiting the maximum frictional force is shown. That is, the size of the tire friction circle is determined by the maximum value of the frictional force between the tire and the contact surface. That is, by plotting the maximum value of the resultant force between the braking / driving power Fx and the lateral force Fy in accordance with the direction of the resultant force, an elliptical tire friction circle can be drawn.
Further, when the external force applied to the tire on the tire contact surface is larger than the tire friction circle, the tire is not in a frictional state with the contact surface, that is, the relative displacement between the tire and the ground increases, so-called Indicates a slip state. This means that the relationship between the tire friction circle and the grip force in the front-rear direction and the lateral direction cannot exhibit the maximum grip force in the front-rear direction and the lateral direction simultaneously.

このようなタイヤ摩擦円と車輪力の大きさとの関係を基に、車輪力の大きさがタイヤ摩擦円の半径(外周)に近づくほど、タイヤが発揮できる摩擦力の最大値(摩擦限界)に近づくと判別できる。すなわち、摩擦限界に対するタイヤのグリップ力の余裕度を判別できる。
以下の説明では、制駆動動力Fx、横力Fy、及び制駆動動力Fxと横力Fyとの合力を総称して車輪力又はタイヤ力と称する。
Based on the relationship between the tire friction circle and the wheel force, the maximum frictional force that can be exerted by the tire (friction limit) increases as the wheel force approaches the radius (outer periphery) of the tire friction circle. It can be identified when approaching. That is, the margin of the grip force of the tire with respect to the friction limit can be determined.
In the following description, the braking / driving power Fx, the lateral force Fy, and the resultant force of the braking / driving power Fx and the lateral force Fy are collectively referred to as wheel force or tire force.

(4)3次元座標を用いた車輪の車輪力、スリップ度、及びタイヤ摩擦円の関係
前述のようなタイヤ摩擦円と車輪力との関係、さらには車輪力と車輪スリップ度(スリップ率λ、スリップ角βt)との関係を基に、3次元座標を用いて車輪の車輪力、スリップ度、及びタイヤ摩擦円の関係を得ることができる。以下に、その関係を示す3次元座標の特性曲線を得る手順を説明する。
(4) Relationship between wheel force, slip degree, and tire friction circle using three-dimensional coordinates Relationship between tire friction circle and wheel force as described above, and further, wheel force and wheel slip degree (slip ratio λ, Based on the relationship with the slip angle βt), the relationship between the wheel force of the wheel, the degree of slip, and the tire friction circle can be obtained using three-dimensional coordinates. A procedure for obtaining a characteristic curve of three-dimensional coordinates indicating the relationship will be described below.

(4−1)3次元座標を用いた車輪の車輪力とスリップ度との関係
図20は、制駆動力Fxとスリップ率λとの関係(2次元座標系)を3次元座標系に変換する手順を示す。図20(a)(前記図1のタイヤ特性曲線(Fx−λ特性曲線)に相当)に示すように、制駆動力Fxが最大値を示すスリップ率λをλpeakと定義する。すなわち、制駆動力Fxはスリップ率λの増加に伴い増加していくが、スリップ率λがある程度大きくなると制駆動力Fxは飽和し、それ以降、逆に低下していく。この制駆動力Fxが飽和するスリップ率λの点(飽和点)をλpeakと定義する。
(4-1) Relationship between Wheel Force and Slip Degree of Wheel Using Three-dimensional Coordinate FIG. 20 converts the relationship (two-dimensional coordinate system) between braking / driving force Fx and slip ratio λ into a three-dimensional coordinate system. Show the procedure. As shown in FIG. 20A (corresponding to the tire characteristic curve (Fx-λ characteristic curve) in FIG. 1), the slip ratio λ at which the braking / driving force Fx has the maximum value is defined as λpeak. That is, the braking / driving force Fx increases as the slip ratio λ increases, but when the slip ratio λ increases to some extent, the braking / driving force Fx saturates and thereafter decreases. A point (saturation point) at which the braking / driving force Fx is saturated is defined as λpeak.

次に、図20(b)に示すように、スリップ率λの軸をλpeakによりλ/λpeakの無次元値にする変換をした後、λ/λpeakが1の値を原点に変更する(制駆動力Fxの軸をλ/λpeakが1の値に移動する)。そして、図20(c)に示すように、図20(b)の2次元座標系を90度回転させる。次いで、図20(d)に示すように、制駆動力Fxとλ/λpeakとの関係線(特性曲線)を3次元座標系の一つの象限上に表す。図20(d)では、λ/λpeakの軸をZ軸としている。Zはスリップ度(スリップ度S)となる。   Next, as shown in FIG. 20B, after converting the axis of the slip ratio λ to a dimensionless value of λ / λpeak by λpeak, the value of λ / λpeak is changed to the origin (braking / braking) The axis of force Fx is moved to a value where λ / λpeak is 1. Then, as shown in FIG. 20C, the two-dimensional coordinate system of FIG. 20B is rotated by 90 degrees. Next, as shown in FIG. 20 (d), a relationship line (characteristic curve) between the braking / driving force Fx and λ / λpeak is represented on one quadrant of the three-dimensional coordinate system. In FIG. 20D, the axis of λ / λpeak is the Z axis. Z is the slip degree (slip degree S).

図21は、横力Fyとスリップ角βtとの関係(2次元座標系)を3次元座標系に変換する手順を示す。この横力Fyとスリップ角βtとの関係でも、制駆動力Fxとスリップ率λとの関係の場合と同様にして3次元座標系に変換している。すなわち、図21(a)(前記図11のタイヤ特性曲線(Fy−βt特性曲線)に相当)に示すように、横力Fyが最大値となるスリップ角βtをβtpeakと定義する。つまり、横力Fyはスリップ角βtの増加に伴い増加していくが、スリップ角βtがある程度大きくなると横力Fyは飽和し、それ以降、逆に低下していく。この横力Fyが飽和するスリップ角βtの点(飽和点)をβtpeakと定義する。   FIG. 21 shows a procedure for converting the relationship (two-dimensional coordinate system) between the lateral force Fy and the slip angle βt into a three-dimensional coordinate system. The relationship between the lateral force Fy and the slip angle βt is also converted into a three-dimensional coordinate system in the same manner as the relationship between the braking / driving force Fx and the slip rate λ. That is, as shown in FIG. 21 (a) (corresponding to the tire characteristic curve (Fy-βt characteristic curve in FIG. 11)), the slip angle βt at which the lateral force Fy becomes the maximum value is defined as βtpeak. That is, the lateral force Fy increases as the slip angle βt increases. However, when the slip angle βt increases to some extent, the lateral force Fy saturates and thereafter decreases. A point (saturation point) of the slip angle βt at which the lateral force Fy is saturated is defined as βtpeak.

次に、図21(b)に示すように、スリップ角βtの軸をβtpeakによりβt/βtpeakの無次元値にする変換をした後、βt/βtpeakが1の値を原点に変更する(横力Fyの軸をβt/βtpeakが1の値に移動する)。そして、図21(c)に示すように、図21(b)の2次元座標系を90度回転させる。次いで、図21(d)に示すように、横力Fyとβt/βtpeakとの関係線(特性曲線)を3次元座標系の一つの象限上に表す。図21(d)では、βt/βtpeakの軸をZ軸としている。   Next, as shown in FIG. 21B, after converting the axis of the slip angle βt to a dimensionless value of βt / βtpeak by βtpeak, the value of βt / βtpeak is changed to the origin (lateral force) The axis of Fy is moved to a value of βt / βtpeak of 1). Then, as shown in FIG. 21 (c), the two-dimensional coordinate system of FIG. 21 (b) is rotated by 90 degrees. Next, as shown in FIG. 21 (d), the relationship line (characteristic curve) between the lateral force Fy and βt / βtpeak is expressed in one quadrant of the three-dimensional coordinate system. In FIG. 21D, the axis of βt / βtpeak is the Z axis.

図22は、前記図20(d)の制駆動力Fxとλ/λpeakとの関係線(特性曲線、Fx−Z面)と、前記図21(d)の横力Fyとβt/βtpeakとの関係線(特性曲線、Fy−Z面)との間を補完して得た3次元曲面を示す。前記図20(d)の制駆動力Fxとλ/λpeakとの関係線(特性曲線)aと前記図21(d)の横力Fyとβt/βtpeakとの関係線(特性曲線)bとの間を、Z軸上の各値で楕円、すなわちタイヤ摩擦円相当で補完して、この図22の3次元曲面を得ている。図22の3次元曲面は、Fx軸及びZ軸を含むFx−Z面とFy軸及びZ軸を含むFy−Z面との間に存在する曲面をなす。   FIG. 22 shows the relationship between the braking / driving force Fx and λ / λpeak in FIG. 20D (characteristic curve, Fx-Z plane) and the lateral force Fy and βt / βtpeak in FIG. A three-dimensional curved surface obtained by interpolating between the relationship lines (characteristic curve, Fy-Z plane) is shown. The relationship line (characteristic curve) a between the braking / driving force Fx and λ / λpeak in FIG. 20D and the relationship line (characteristic curve) b between the lateral force Fy and βt / βtpeak in FIG. The three-dimensional curved surface of FIG. 22 is obtained by complementing the gap with each value on the Z axis by an ellipse, that is, equivalent to a tire friction circle. The three-dimensional curved surface of FIG. 22 forms a curved surface that exists between the Fx-Z plane including the Fx axis and the Z axis and the Fy-Z plane including the Fy axis and the Z axis.

この図22では、単位が異なるスリップ率λとスリップ角βtとをそれぞれλ/λpeak及びβt/βtpeakの無次元値にすることで、スリップ率λとスリップ角βtとを同じ座標軸のZ軸に表現している。そして、前述のように、スリップ率λとスリップ角βtとを総称する概念がスリップ度(Z)となる。このようなことから、図22のZ軸は、スリップ度(λ/λpeak,βt/βtpeak)を示す軸となる。
よって、3次元曲面は、スリップ度と車輪力(タイヤ力)との相関関係を表すものとなる。また、この3次元曲面は、制駆動力Fxと横力Fyとの合力Fと、合力Fに起因して発生するスリップ度Zとの関係線の集合から構成されるものとなる。
In FIG. 22, the slip ratio λ and the slip angle βt, which are different units, are set to dimensionless values of λ / λpeak and βt / βtpeak, respectively, so that the slip ratio λ and the slip angle βt are expressed on the same coordinate axis Z-axis. is doing. As described above, the concept that collectively refers to the slip ratio λ and the slip angle βt is the slip degree (Z). For this reason, the Z-axis in FIG. 22 is an axis indicating the slip degree (λ / λpeak, βt / βtpeak).
Therefore, the three-dimensional curved surface represents the correlation between the slip degree and the wheel force (tire force). The three-dimensional curved surface is composed of a set of relational lines between the resultant force F of the braking / driving force Fx and the lateral force Fy and the slip degree Z generated due to the resultant force F.

ここで、合力Fは、制駆動力Fx及び横力Fyを成分としてタイヤ斜め方向に発生している力に相当する。よって、制駆動力Fxが零であれば、合力Fは横力Fyそのものになり、横力Fyが零であれば、合力Fは制駆動力Fxそのものになる。また、合力Fに起因して発生するスリップ度Zとは、スリップ率λ及びスリップ角βtを合成した値、又はスリップ率λ及びスリップ角βtを成分とする値の概念である。よって、スリップ率λが零であれば、スリップ度Zはスリック角βtそのものになり、スリップ角βtが零であれば、スリップ度Zはスリップ率λそのものになる。   Here, the resultant force F corresponds to a force generated in the tire oblique direction using the braking / driving force Fx and the lateral force Fy as components. Therefore, if the braking / driving force Fx is zero, the resultant force F is the lateral force Fy itself, and if the lateral force Fy is zero, the resultant force F is the braking / driving force Fx itself. The slip degree Z caused by the resultant force F is a concept of a value obtained by combining the slip ratio λ and the slip angle βt, or a value having the slip ratio λ and the slip angle βt as components. Therefore, if the slip ratio λ is zero, the slip degree Z is the slick angle βt itself, and if the slip angle βt is zero, the slip degree Z is the slip ratio λ itself.

なお、図22では、スリップ度と車輪力との関係を表す3次元曲面を、1/4周分(1/4象限)強しか表示していない。しかし、実際には、スリップ度と車輪力との相関関係を表す3次元曲面は、全周分存在し、ドーム状又は半球状になる。
図23は、前記図22が、制駆動力Fxと横力Fyとの合力Fと、合力Fに起因して発生するスリップ度Zとの関係線(2次元特性曲線)の集合から構成されることを説明する図である。3次元座標系における合力Fの大きさ・向きは、制駆動力Fxのスカラ量・向きと横力Fyのスカラ量・向きとの異なる組み合わせにより、無数に存在する。この実施形態では、車輪力(F)は、Z軸回り360度全周の何れの方向でも良く、図示の実施形態では全方向に対応している。これにより、図23(a)に示す3次元座標系における、合力Fと該合力Fに起因して発生するスリップ度Zとの関係は、Z軸と合力Fとを含む平面に表された2次元特性の集合からなると言える。つまり、図23(b)に示すように、合力Fと該合力Fに起因して発生するスリップ度Zとの関係を2次元特性曲線として得ることができる。すなわち、Z軸と合力Fとを含む平面は、合力の方向に応じて、Z軸のまわりに無数に存在し、それら無数の平面は、Z軸を軸として平面束(asheaf of planes)を成している。そして、その平面の各々に図23(b)のような2次元特性曲線が存在する。
In FIG. 22, the three-dimensional curved surface representing the relationship between the slip degree and the wheel force is displayed only for a quarter of a quarter (quarter quadrant). However, in practice, a three-dimensional curved surface that represents the correlation between the slip degree and the wheel force exists for the entire circumference, and has a dome shape or a hemispherical shape.
FIG. 23 shows that FIG. 22 is composed of a set of relation lines (two-dimensional characteristic curves) between the resultant force F of the braking / driving force Fx and the lateral force Fy and the slip degree Z generated due to the resultant force F. It is a figure explaining this. The magnitude / direction of the resultant force F in the three-dimensional coordinate system is infinite due to different combinations of the scalar amount / direction of the braking / driving force Fx and the scalar amount / direction of the lateral force Fy. In this embodiment, the wheel force (F) may be in any direction 360 degrees around the Z axis, and corresponds to all directions in the illustrated embodiment. Thereby, in the three-dimensional coordinate system shown in FIG. 23A, the relationship between the resultant force F and the slip degree Z generated due to the resultant force F is expressed in a plane including the Z axis and the resultant force F. It can be said that it consists of a set of dimensional characteristics. That is, as shown in FIG. 23 (b), the relationship between the resultant force F and the slip degree Z generated due to the resultant force F can be obtained as a two-dimensional characteristic curve. That is, there are an infinite number of planes including the Z axis and the resultant force F around the Z axis according to the direction of the resultant force, and these infinite planes form an asheaf of planes around the Z axis. is doing. A two-dimensional characteristic curve as shown in FIG. 23B exists on each of the planes.

図23を用いて、合力Fについての摩擦限界までの余裕度を3次元座標系上で説明する。図23(a)に示す、スリップ度と車輪力(Fx,Fy,F)との関係を表す3次元曲面と、合力FのベクトルとZ軸とを含む平面との交線として、図23(b)に示すタイヤ特性曲線を得ることができる。このようして得た図23(b)のタイヤ特性曲線の接線の傾きが、タイヤの摩擦限界までの余裕度を示すものとなる。すなわち、図23(b)のタイヤ特性曲線の接線の傾きが正値から零に近づくと、タイヤの摩擦限界に近くなる。よって、このタイヤ特性曲線の接線の傾きを検出できれば、摩擦限界に到る前の状態において、摩擦限界までの余裕度を知ることができる。また、図23(b)のタイヤ特性曲線の接線の傾きが負値となると、摩擦力が飽和した状態、いわゆるスリップ状態になる。この点では、タイヤ特性曲線の接線の傾きを検出できれば、スリップ状態に到る前に摩擦限界(摩擦力が飽和する)までの余裕度を知ることができると言える。   The margin to the friction limit for the resultant force F will be described on the three-dimensional coordinate system with reference to FIG. As an intersection line between the three-dimensional curved surface representing the relationship between the slip degree and the wheel force (Fx, Fy, F) and the plane including the vector of the resultant force F and the Z axis shown in FIG. The tire characteristic curve shown in b) can be obtained. The slope of the tangent line of the tire characteristic curve of FIG. 23 (b) obtained in this way indicates the margin to the tire friction limit. That is, when the slope of the tangent line of the tire characteristic curve in FIG. 23B approaches zero from a positive value, the tire approaches the friction limit. Therefore, if the inclination of the tangent line of the tire characteristic curve can be detected, it is possible to know the margin to the friction limit in the state before reaching the friction limit. Further, when the tangent slope of the tire characteristic curve in FIG. 23B becomes a negative value, the frictional force is saturated, that is, a so-called slip state. In this respect, if the slope of the tangent line of the tire characteristic curve can be detected, it can be said that the margin to the friction limit (friction force is saturated) can be known before the slip state is reached.

図24は、タイヤ摩擦円の大きさが変化する場合の合力Fと該合力Fに起因して発生するスリップ度Zとの関係を示す。タイヤ摩擦円の大きさは、前述のように、タイヤと接地面との間の摩擦力の最大値(以下、最大摩擦力という。)によって決まる。すなわち、タイヤと接地面との間の摩擦力の最大値が小さくなると、タイヤ摩擦円も小さくなる。このようなことから、実際には路面μが変化すること等により、図24(a)及び(b)に示すように、タイヤ特性曲線(タイヤ摩擦円)が、最大摩擦力の大きさによって変化するようになる。   FIG. 24 shows the relationship between the resultant force F when the size of the tire friction circle changes and the slip degree Z generated due to the resultant force F. As described above, the size of the tire friction circle is determined by the maximum value of the frictional force between the tire and the ground contact surface (hereinafter referred to as the maximum frictional force). That is, when the maximum value of the frictional force between the tire and the contact surface is reduced, the tire friction circle is also reduced. For this reason, the tire characteristic curve (tire friction circle) changes depending on the magnitude of the maximum frictional force, as shown in FIGS. 24 (a) and 24 (b), due to actual changes in the road surface μ. To come.

図25は、最大摩擦力、すなわち路面μが異なるタイヤ特性曲線(F−Z特性曲線)と、原点O(スリップ度と車輪力がともに零である点)を通る直線(一点鎖線で示す直線)との関係を示す。図25(a)及び図25(b)に示すように、路面μが異なるタイヤ特性曲線について、直線との交点での接線の傾き(μ勾配)は同一となる。すなわち、最大摩擦力が異なるタイヤ特性曲線について、合力Fとスリップ度Zとの比(F/Z)が同一であれば、接線の傾きは同一となる。   FIG. 25 shows a tire characteristic curve (FZ characteristic curve) having different maximum frictional force, that is, road surface μ, and a straight line (a straight line indicated by a one-dot chain line) passing through the origin O (a point where both the slip degree and the wheel force are zero). Shows the relationship. As shown in FIGS. 25 (a) and 25 (b), the tire characteristic curves with different road surface μ have the same tangential slope (μ gradient) at the intersection with the straight line. That is, if the ratio (F / Z) between the resultant force F and the slip degree Z is the same for tire characteristic curves having different maximum frictional forces, the tangential slopes are the same.

そして、各タイヤ特性曲線(F−Z特性曲線)で合力Fとスリップ度Zとの比(F/Z)が同一となる値(Z,F)に関し、異なるタイヤ特性曲線で得られる合力F同士の比又はスリップ度Z同士の比は、路面μの比と等しくなる。すなわち、該合力F同士の比又は該スリップ度Z同士の比が知ることができれば、路面μの比を知ることができる。
図26を用いて、路面μが異なる各タイヤ特性曲線について、合力F同士の比又はスリップ度Z同士の比と、その路面μの比との関係を説明する。
Then, with respect to the values (Z, F) at which the ratio (F / Z) of the resultant force F and the slip degree Z is the same in each tire characteristic curve (FZ characteristic curve), the resultant forces F obtained with different tire characteristic curves Or the ratio between the slip degrees Z is equal to the ratio of the road surface μ. That is, if the ratio between the resultant forces F or the ratio between the slip degrees Z can be known, the ratio of the road surface μ can be known.
26, the relationship between the ratio of the resultant force F or the ratio of the slip degree Z and the ratio of the road surface μ will be described for each tire characteristic curve having a different road surface μ.

図26(a)におけるある合力Fとスリップ度Zとの関係(2次元のタイヤ特性曲線)を取り出した図26(b)に示すように、合力Fとスリップ度Zとの比(F/Z)が同一となる値(Z,F)(同図中に■印、●印でそれぞれ示す値)でそれぞれ得られる横力a2と横力b2との比(a2/b2)と、路面Aの路面μ値μと路面Bの路面μ値μとの比(μ/μ)とは同一値になる。 As shown in FIG. 26 (b) in which the relationship (two-dimensional tire characteristic curve) between a certain resultant force F and slip degree Z in FIG. 26 (a) is extracted, the ratio (F / Z) of the resultant force F and slip degree Z is shown. ) Are the same values (Z, F) (values indicated by ■ and ● in the figure), respectively, and the ratio (a2 / b2) between the lateral force a2 and the lateral force b2 and the road surface A It becomes the same value as the ratio of the road surface mu values mu B of the road surface mu values mu a and the road surface B (μ a / μ B) .

また、同じく、合力Fとスリップ度Zとの比(F/Z)が同一となる値(Z,F)でそれぞれ得られるスリップ度a3とスリップ度b3との比(a3/b3)と、路面Aの路面μ値μと路面Bの路面μ値μとの比(μ/μ)とは同一値になる。
このようなことから、路面Aで得られるタイヤ特性曲線と路面Bで得られるタイヤ特性曲線とで、合力Fとスリップ度Zとの比(F/Z)が同一となる値(Z,F)と原点(0,0)とをそれぞれ結んで得られる線長a1と線長b1との比(a1/b1)と、路面Aの路面μ値μと路面Bの路面μ値μとの比(μ/μ)とは同一値になる。このことは、幾何学的に次のように証明できる。
Similarly, the ratio (a3 / b3) of the slip degree a3 and the slip degree b3 obtained at values (Z, F) at which the ratio (F / Z) of the resultant force F and the slip degree Z is the same, and the road surface becomes the same value as the ratio of the road surface mu values mu B of a of road surface mu values mu a and the road surface B (μ a / μ B) .
Therefore, the tire characteristic curve obtained on the road surface A and the tire characteristic curve obtained on the road surface B have the same ratio (F / Z) between the resultant force F and the slip degree Z (F, Z). and the origin (0, 0) ratio and the a line length a1 and line length b1 obtained by connecting each (a1 / b1), a road surface a of road surface mu values mu a and the road surface B road mu values of mu B The ratio (μ A / μ B ) is the same value. This can be proved geometrically as follows.

路面Aのタイヤ特性曲線を用いて得られる三角形(a1,a2,a3を辺とする三角形)と路面Bのタイヤ特性曲線を用いて得られる三角形(b1,b2,b3を辺とする三角形)とは相似の三角形となる。このことから、a1とb1との比と、a2とb2との比と、a3とb3との比とは、それぞれ同一値になる(a1:b1=a2:b2=a3:b3)。そして、合力Fについてのa2とb2との比及びスリップ度Zについてのa3とb3との比は、路面Aの路面μ値μと路面Bの路面μ値μとの比(μ/μ)と同一値になる。よって、前述のように、線長a1と線長b1との比(a1/b1)と、路面Aの路面μ値μと路面Bの路面μ値μとの比(μ/μ)とは同一値となる結論を得ることができる。 A triangle (triangle with sides a1, a2 and a3) obtained using the tire characteristic curve of road surface A and a triangle (triangle with sides b1, b2 and b3) obtained using the tire characteristic curve of road surface B, and Becomes a similar triangle. From this, the ratio of a1 and b1, the ratio of a2 and b2, and the ratio of a3 and b3 are the same value (a1: b1 = a2: b2 = a3: b3). The ratio of a2 and b2 for the resultant force F and the ratio of a3 and b3 for the slip degree Z are the ratio of the road surface μ value μ A of the road surface A and the road surface μ value μ B of the road surface B (μ A / μ B ) and the same value. Therefore, as described above, the ratio between the line length a1 and the line length b1 (a1 / b1) and the ratio between the road surface μ value μ A of the road surface A and the road surface μ value μ B of the road surface B (μ A / μ B ) Can be concluded to be the same value.

図27は、一例として、前記線長を基に走行路面の路面μを算出する演算手順を示す。ここでは、ある走行路面Bで得た合力Fyb及びスリップ度Zbを基に、既知の路面Aの路面μ値μのタイヤ特性曲線を参照して、ある走行路面Bの路面μ値μを算出する例を示す。
図27に示すように、先ずステップS21及びステップS22において、ある走行路面Bでの合力Fb及びスリップ度Zbを検出する。続いてステップS23において、路面μ値μの路面Aのタイヤ特性曲線の原点(0,0)と実測点(Zb,Fb)とを通る直線が、そのタイヤ特性曲線と交わる点の値(Za,Fa)を特定する。
FIG. 27 shows a calculation procedure for calculating the road surface μ of the traveling road surface based on the line length as an example. Here, based on the resultant force Fyb and slip degree Zb obtained on a certain road surface B, a road surface μ value μ B of a certain road surface B is obtained by referring to a tire characteristic curve of a road surface μ value μ A of a known road surface A. An example of calculation is shown.
As shown in FIG. 27, first, in step S21 and step S22, the resultant force Fb and slip degree Zb on a certain road surface B are detected. Subsequently, in step S23, the origin of the tire characteristic curve of the road surface A of road surface mu values mu A (0,0) and the measured point (Zb, Fb) and a straight line, the value of the point of intersection with the tire characteristic curve passing through (Za , Fa).

続いてステップS24において、ある走行路面Bの路面μ値μを算出(推定)する。すなわち、前記実測点(Zb,Fb)と路面Aのタイヤ特性曲線の原点とを結ぶ直線の線長b1(=√(Zb+Fb))を得る。また、前記ステップS23で特定した路面Aのタイヤ特性曲線の交点の値(Za,Fa)と該タイヤ特性曲線の原点とを結ぶ直線の線長a1(=√(Za+Fa))を得る。さらに、線長b1と線長a1との比(b1/a1)を算出する。そして、その算出した比(b1/a1)と、路面Aの路面μ値μとを乗算し、その乗算値を走行路面Bの路面μ値μとして得る(μ=μ・b1/a1)。 Subsequently, in step S24, a road surface μ value μ B of a certain traveling road surface B is calculated (estimated). That is, a straight line length b1 (= √ (Zb 2 + Fb 2 )) connecting the actual measurement point (Zb, Fb) and the origin of the tire characteristic curve of the road surface A is obtained. Further, the straight line length a1 (= √ (Za 2 + Fa 2 )) connecting the intersection value (Za, Fa) of the tire characteristic curve on the road surface A specified in step S23 and the origin of the tire characteristic curve is obtained. . Further, the ratio (b1 / a1) between the line length b1 and the line length a1 is calculated. Then, its calculated ratio (b1 / a1), multiplying the road surface mu values mu A of road surface A, to obtain the multiplied value as the road surface mu value mu B of road surface B (μ B = μ A · b1 / a1).

(4−2)3次元座標を用いた車輪の車輪力とグリップ状態(μ勾配)との関係
合力Fとスリップ度Zとの比(F/Z)とタイヤ特性曲線の接線の傾き(μ勾配)との関係を、最大摩擦力に依存しない形で整理できる。
図28は、合力Fとスリップ度Zとの比(F/Z)と、タイヤ特性曲線の接線の傾きとの関係を示す。図28に示すように、合力Fとスリップ度Zとの比(F/Z)とタイヤ特性曲線の接線の傾きとの関係を整理することで、最大摩擦力に依存しない一つの特性(2次元特性曲線)に集約することができる。よって、図28に示すような特性データを予め準備しておく。例えば特性マップとして準備しておく。そして、合力Fとスリップ度Zとがわかれば、特性データを用いることで、タイヤ特性曲線の接線の傾きの値を知ることができ、摩擦限界に対する余裕度を判定できる。すなわち、最大摩擦力の情報を得ることなく(最大摩擦力を推定することなく)、摩擦限界に対する余裕度を判定できる。
以上のように、車輪の車輪力、スリップ度、及びタイヤ摩擦円の関係を3次元座標系の特性として得ることができる。さらに、合力Fとスリップ度Zとの比(F/Z)とタイヤ特性曲線の接線の傾き(μ勾配)との関係を2次元座標系の特性(μ勾配特性)として得ることができる。
(4-2) Relationship between wheel force and grip state (μ gradient) using three-dimensional coordinates Ratio of resultant force F to slip degree (F / Z) and slope of tangent to tire characteristic curve (μ gradient) ) With the maximum frictional force.
FIG. 28 shows the relationship between the ratio (F / Z) between the resultant force F and the slip degree Z and the tangent slope of the tire characteristic curve. As shown in FIG. 28, by arranging the relationship between the ratio (F / Z) of the resultant force F and the slip degree Z and the slope of the tangent to the tire characteristic curve, one characteristic (two-dimensional) that does not depend on the maximum frictional force is obtained. Characteristic curve). Therefore, characteristic data as shown in FIG. 28 is prepared in advance. For example, it is prepared as a characteristic map. If the resultant force F and the slip degree Z are known, the characteristic data can be used to know the value of the tangent slope of the tire characteristic curve, and the margin with respect to the friction limit can be determined. That is, the margin with respect to the friction limit can be determined without obtaining information on the maximum friction force (without estimating the maximum friction force).
As described above, the relationship between the wheel force of the wheel, the slip degree, and the tire friction circle can be obtained as the characteristics of the three-dimensional coordinate system. Furthermore, the relationship between the ratio (F / Z) between the resultant force F and the slip degree Z and the slope of the tangent to the tire characteristic curve (μ gradient) can be obtained as a characteristic of the two-dimensional coordinate system (μ gradient characteristic).

(実施形態)
以上の技術の採用により実現した実施形態を次に説明する。
(構成)
本実施形態は、本発明を適用した車両である。図29は、車両の概略構成を示す。図29に示すように、車両は、操舵角センサ1、ヨーレイトセンサ2、横加速度センサ3、前後加速度センサ4、車輪速センサ5、EPSECU(ElectricPower Steering Electronic Control Unit)6、EPS(Electric Power Steering)モータ7及び車両走行状態推定装置8を備える。さらに、車両は、各車輪11FL〜11RRに直結した制駆動モータ21FL〜21RR、制駆動モータECU(ElectronicControl Unit)22を有する。
(Embodiment)
Next, an embodiment realized by adopting the above technique will be described.
(Constitution)
The present embodiment is a vehicle to which the present invention is applied. FIG. 29 shows a schematic configuration of the vehicle. As shown in FIG. 29, the vehicle includes a steering angle sensor 1, a yaw rate sensor 2, a lateral acceleration sensor 3, a longitudinal acceleration sensor 4, a wheel speed sensor 5, an EPS ECU (Electric Power Steering Electronic Control Unit) 6, and an EPS (Electric Power Steering). A motor 7 and a vehicle running state estimation device 8 are provided. Further, the vehicle has braking / driving motors 21 FL to 21 RR and braking / driving motor ECUs (Electronic Control Units) 22 directly connected to the wheels 11 FL to 11 RR .

操舵角センサ1は、ステアリングホイール9と一体に回転するステアリングシャフト10の回転角を検出する。操舵角センサ1は、その検出結果(操舵角)を車両走行状態推定装置8に出力する。ヨーレイトセンサ2は、車両のヨーレイトを検出する。ヨーレイトセンサ2は、その検出結果を車両走行状態推定装置8に出力する。横加速度センサ3は、車両の横加速度を検出する。横加速度センサ3は、その検出結果を車両走行状態推定装置8に出力する。前後加速度センサ4は、車両の前後加速度を検出する。前後加速度センサ4は、その検出結果を車両走行状態推定装置8に出力する。車輪速センサ5は、車体に設けられた各車輪11FL〜11RRの車輪速を検出する。車輪速センサ5は、その検出結果を車両走行状態推定装置8に出力する。 The steering angle sensor 1 detects the rotation angle of the steering shaft 10 that rotates integrally with the steering wheel 9. The steering angle sensor 1 outputs the detection result (steering angle) to the vehicle running state estimation device 8. The yaw rate sensor 2 detects the yaw rate of the vehicle. The yaw rate sensor 2 outputs the detection result to the vehicle running state estimation device 8. The lateral acceleration sensor 3 detects the lateral acceleration of the vehicle. The lateral acceleration sensor 3 outputs the detection result to the vehicle running state estimation device 8. The longitudinal acceleration sensor 4 detects the longitudinal acceleration of the vehicle. The longitudinal acceleration sensor 4 outputs the detection result to the vehicle running state estimation device 8. The wheel speed sensor 5 detects wheel speeds of the wheels 11 FL to 11 RR provided on the vehicle body. The wheel speed sensor 5 outputs the detection result to the vehicle running state estimation device 8.

EPSECU6は、操舵角センサ1が検出した操舵角を基に、操舵アシスト指令をEPSモータ7に出力する。ここでいう操舵アシスト指令は、操舵力アシストを行うための指令信号である。また、EPSECU6は、車両走行状態推定装置8が出力する指令値(不安定挙動抑制アシスト指令)を基に、操舵アシスト指令をEPSモータ7に出力する。ここでいう操舵アシスト指令は、車両の不安定挙動を抑制するための指令信号である。   The EPS ECU 6 outputs a steering assist command to the EPS motor 7 based on the steering angle detected by the steering angle sensor 1. The steering assist command here is a command signal for performing steering force assist. Further, the EPS ECU 6 outputs a steering assist command to the EPS motor 7 based on the command value (unstable behavior suppression assist command) output by the vehicle running state estimation device 8. The steering assist command here is a command signal for suppressing the unstable behavior of the vehicle.

EPSモータ7は、EPSECU6が出力する操舵アシスト指令を基に、ステアリングシャフト10に回転トルクを付与する。これにより、EPSモータ7は、ステアリングシャフト10に連結されているラック・アンド・ピニオン機構(ピニオン12、ラック13)、タイロッド14及びナックルアームを介して左右の前輪11FL,11FRの転舵を補助する。
制駆動モータECU22は、ブレーキペダル15及びアクセルペダル16からのドライバ入力、並びに車両走行状態推定装置8からの情報を基に、制駆動モータ21FL〜21RRを制御する。
The EPS motor 7 applies rotational torque to the steering shaft 10 based on a steering assist command output from the EPS ECU 6. Thereby, the EPS motor 7 steers the left and right front wheels 11 FL and 11 FR via the rack and pinion mechanism (pinion 12 and rack 13) connected to the steering shaft 10, the tie rod 14 and the knuckle arm. Assist.
The braking / driving motor ECU 22 controls the braking / driving motors 21 FL to 21 RR based on driver inputs from the brake pedal 15 and the accelerator pedal 16 and information from the vehicle running state estimation device 8.

車両走行状態推定装置8は、操舵角センサ1、ヨーレイトセンサ2、横加速度センサ3、前後加速度センサ4及び車輪速センサ5の検出結果等を基に、車両の走行状態を推定する。車両走行状態推定装置8は、その推定結果を基に、指令値(不安定挙動抑制アシスト指令)をEPSECU6及び制駆動モータECU22に出力する。ここでいう指令値は、車両の不安定挙動を抑制するようにEPSモータ7や制駆動力を制御するための指令信号である。   The vehicle travel state estimation device 8 estimates the travel state of the vehicle based on the detection results of the steering angle sensor 1, the yaw rate sensor 2, the lateral acceleration sensor 3, the longitudinal acceleration sensor 4, and the wheel speed sensor 5. The vehicle running state estimation device 8 outputs a command value (unstable behavior suppression assist command) to the EPS ECU 6 and the braking / driving motor ECU 22 based on the estimation result. The command value here is a command signal for controlling the EPS motor 7 and the braking / driving force so as to suppress the unstable behavior of the vehicle.

図30は、車両走行状態推定装置8の構成を示す。図30に示すように、車両走行状態推定装置8は、車体速度演算部41、車体スリップ角推定部42、タイヤスリップ角演算部43、スリップ率演算部44及び路面μ推定値演算部45を有する。また、この車両は、タイヤ力センサ46を有する。
車体速度演算部41は、車輪速センサ5が検出した車輪速及び前後加速度センサ4が検出した前後加速度を基に、車体速度を推定する。具体的には、車体速度演算部41は、従動輪11RL,11RRの車輪速の平均値、又は各車輪11FL〜11RRの車輪速の平均値を算出して、その算出値を車体速度の基本値としている。車体速度演算部41は、その基本値を前後加速度により補正する。具体的には、その基本値から急加速時のタイヤ空転や急制動時のタイヤロックによる誤差の影響を除くように補正をする。車体速度演算部41は、その補正した値を車体速度の推定結果とする。車体速度演算部41は、その推定結果を車体スリップ角推定部42に出力する。
FIG. 30 shows the configuration of the vehicle running state estimation device 8. As shown in FIG. 30, the vehicle running state estimation device 8 includes a vehicle body speed calculation unit 41, a vehicle body slip angle estimation unit 42, a tire slip angle calculation unit 43, a slip ratio calculation unit 44, and a road surface μ estimated value calculation unit 45. . The vehicle also has a tire force sensor 46.
The vehicle body speed calculation unit 41 estimates the vehicle body speed based on the wheel speed detected by the wheel speed sensor 5 and the longitudinal acceleration detected by the longitudinal acceleration sensor 4. Specifically, the vehicle body speed calculation unit 41 calculates the average value of the wheel speeds of the driven wheels 11 RL and 11 RR or the average value of the wheel speeds of the wheels 11 FL to 11 RR , and uses the calculated value as the vehicle body. This is the basic value of speed. The vehicle body speed calculation unit 41 corrects the basic value by the longitudinal acceleration. Specifically, correction is made from the basic value so as to eliminate the influence of errors caused by tire slipping during sudden acceleration and tire lock during sudden braking. The vehicle body speed calculation unit 41 uses the corrected value as the estimation result of the vehicle body speed. The vehicle body speed calculation unit 41 outputs the estimation result to the vehicle body slip angle estimation unit 42.

車体スリップ角推定部42は、操舵角センサ1が検出した操舵角、ヨーレイトセンサ2が検出したヨーレイト、横加速度センサ3が検出した横加速度、前後加速度センサ4が検出した前後加速度及び車体速度演算部41が算出した車体速度を基に、車両の横滑り角(スリップ角)を推定する。
図31は、車体スリップ角推定部42の構成例を示す。図31に示すように、車体スリップ角推定部42は、車両の状態量(車両の横滑り角β、スリップ角β)を推定する線形2入力オブザーバ51を備える。これにより、車体スリップ角推定部42は、車両の横滑り角(スリップ角)βを推定する。ここで、車両の2輪モデルを基に線形2入力オブザーバ51を構築している。その車両の2輪モデルを、車両の横方向の力とモーメントの釣り合いより、下記(1)式で表すことができる。
The vehicle body slip angle estimation unit 42 includes a steering angle detected by the steering angle sensor 1, a yaw rate detected by the yaw rate sensor 2, a lateral acceleration detected by the lateral acceleration sensor 3, a longitudinal acceleration detected by the longitudinal acceleration sensor 4, and a vehicle body speed calculation unit. Based on the vehicle body speed calculated by 41, the side slip angle (slip angle) of the vehicle is estimated.
FIG. 31 shows a configuration example of the vehicle body slip angle estimation unit 42. As shown in FIG. 31, the vehicle body slip angle estimation unit 42 includes a linear two-input observer 51 that estimates a vehicle state quantity (a vehicle side slip angle β, a slip angle β). As a result, the vehicle body slip angle estimation unit 42 estimates the side slip angle (slip angle) β of the vehicle. Here, a linear two-input observer 51 is constructed based on a two-wheel model of the vehicle. The two-wheel model of the vehicle can be expressed by the following equation (1) from the balance between the lateral force and moment of the vehicle.

Figure 2010195327
Figure 2010195327

ここで、A,B,C,Dは車両の線形2輪モデルによって決まる行列である。また、タイヤ舵角を入力uとし、ヨーレイトと横加速度とを出力yとすると、前記(1)式の状態方程式(出力方程式)は、下記(2)式のようになる。   Here, A, B, C, and D are matrices determined by the linear two-wheel model of the vehicle. When the tire rudder angle is input u, and the yaw rate and lateral acceleration are output y, the state equation (output equation) of the equation (1) is as shown in the following equation (2).

Figure 2010195327
Figure 2010195327

ここで、mは車両質量である。Iはヨー慣性モーメントである。lは車両重心点と前車軸間の距離である。lは車両重心点と後車軸間の距離である。Cpは前輪コーナリングパワー(左右輪合計値)である。Cpは後輪コーナリングパワー(左右輪合計値)である。Vは車体速度である。βは車両の横滑り角である。γはヨーレイトである。Gは横加速度である。a11,a12,bは行列A、Bの各要素である。 Here, m is the vehicle mass. I is the yaw moment of inertia. l f is the distance between the vehicle center of gravity and the front axle. l r is the distance between the vehicle center of gravity and the rear axle. The cp f is the front wheel cornering power (right and left wheels total). Cp r is the rear wheel cornering power (the left and right wheels total value). V is the vehicle speed. β is the side slip angle of the vehicle. γ is the yaw rate. G y is the lateral acceleration. a 11 , a 12 , b 1 are the elements of the matrices A and B.

そして、この状態方程式を基に、ヨーレイトと横加速度とを入力とし、オブザーバゲインK1として、線形2入力オブザーバ51を作成する。ここで、オブザーバゲインK1は、モデル化誤差の影響を受けにくく且つ安定した推定を行えるように設定した値である。
また、線形2入力オブザーバ51は、積分器52の入力を補正するβ推定補償器53を備える。これにより、線形2入力オブザーバ51は、限界領域においても推定精度を確保することができる。すなわち、β推定補償器53を備えることで、車両の2輪モデルの設計時に想定した路面状況で且つタイヤの横滑り角が非線形特性とはならない線形域だけでなく、路面μ変化時や限界走行時にあっても横滑り角βを精度よく推定できる。
Based on this state equation, the yaw rate and the lateral acceleration are input, and a linear two-input observer 51 is created as the observer gain K1. Here, the observer gain K1 is a value set so as to be less susceptible to modeling errors and perform stable estimation.
The linear two-input observer 51 includes a β estimation compensator 53 that corrects the input of the integrator 52. Thereby, the linear two-input observer 51 can ensure estimation accuracy even in the limit region. In other words, by including the β estimation compensator 53, not only in the road surface condition assumed at the time of designing the two-wheel model of the vehicle and in the linear region where the tire side slip angle does not become a non-linear characteristic, but also when the road surface μ changes or when the vehicle travels marginally. Even if it exists, the side slip angle β can be estimated with high accuracy.

図32は、車体横滑り角βで走行している旋回中の車両を示す。図32に示すように、車体に働く場の力、つまり旋回中心から外側に向かって働く遠心力も、車幅方向から横滑り角β分ずれた方向に発生する。そのため、β推定補償器53は、下記(3)式に従って場の力のずれ分βを算出する。このずれ分βは、線形2入力オブザーバ51が推定した車両の横滑り角βに補正をかけるときの基準値(目標値)Gとなる。 FIG. 32 shows a turning vehicle running at a vehicle body side slip angle β. As shown in FIG. 32, the field force acting on the vehicle body, that is, the centrifugal force acting outward from the turning center is also generated in a direction shifted by the side slip angle β from the vehicle width direction. Therefore, the β estimation compensator 53 calculates a field force deviation β 2 according to the following equation (3). This deviation β 2 becomes a reference value (target value) G for correcting the vehicle slip angle β estimated by the linear two-input observer 51.

Figure 2010195327
Figure 2010195327

ここで、Gは前後加速度である。また、図33に示すように、速度変化による力の釣り合いも考慮する。これにより、旋回によるもののみを抽出すると、前記(3)式を、下記(4)式として表すことができる。 Here, G x is the longitudinal acceleration. Also, as shown in FIG. 33, force balance due to speed change is also taken into consideration. Thereby, when only the thing by turning is extracted, the said (3) Formula can be represented as following (4) Formula.

Figure 2010195327
Figure 2010195327

そして、β推定補償器53は、その目標値βを線形2入力オブザーバ51が推定した横滑り角βから減算する。さらに、β推定補償器53は、その減算結果に、図34の制御マップによって設定した補償ゲインK2を乗算する。そして、β推定補償器53は、その乗算結果を積分器52の入力としている。
図34の制御マップでは、車両の横方向加速度Gの絶対値(|G|)が第1しきい値以下である場合、補償ゲインK2が零となる。また、車両の横方向加速度Gの絶対値が第1しきい値よりも大きい第2しきい値以上の場合、補償ゲインK2が比較的大きい一定値となる。また、車両の横方向加速度Gの絶対値が第1しきい値と第2しきい値との間にある場合、横方向加速度Gの絶対値が大きくなるほど、補償ゲインK2が大きくなる。
Then, the β estimation compensator 53 subtracts the target value β 2 from the sideslip angle β estimated by the linear two-input observer 51. Further, the β estimation compensator 53 multiplies the subtraction result by the compensation gain K2 set by the control map of FIG. Then, the β estimation compensator 53 uses the multiplication result as an input of the integrator 52.
In the control map of FIG. 34, when the absolute value (| G y |) of the lateral acceleration G y of the vehicle is equal to or smaller than the first threshold value, the compensation gain K2 is zero. Further, if the absolute value of lateral acceleration G y of the vehicle is of the second or more threshold greater than the first threshold value, the compensation gain K2 is relatively large constant value. Further, when the absolute value of lateral acceleration G y of the vehicle is between the first threshold and the second threshold value, the absolute value becomes larger in the lateral acceleration G y, compensation gain K2 is increased.

このように、図34の制御マップでは、横方向加速度Gの絶対値が第1しきい値以下で零近傍の値となる場合、補償ゲインK2を零としている。これにより、直進時のように旋回Gが発生しない状況下では補正をする必要がないことから、誤って補正が行われないようにしている。また、図34の制御マップでは、横方向加速度Gの絶対値が増加して第1しきい値より大きくなると(例えば、0.1Gより大きくなると)、横方向加速度Gの絶対値に比例してフィードバックゲイン(補償ゲイン)K2を増大させていき、横方向加速度Gの絶対値が第2しきい値以上になると(例えば0.5G以上になると)、補償ゲインK2を制御の安定する一定値としている。このようにすることで、横滑り角βの推定精度を向上させている。 Thus, in the control map of FIG. 34, when the absolute value of lateral acceleration G y has a value close to zero or less the first threshold value, and the compensation gain K2 is zero. Thereby, since it is not necessary to correct | amend under the condition where the turning G does not generate | occur | produce like the time of straight running, it is trying not to correct by mistake. Further, in the control map of FIG. 34, when the absolute value of lateral acceleration G y is greater than the first threshold value increases (e.g., becomes greater than 0.1 G), proportional to the absolute value of lateral acceleration G y and gradually increases the feedback gain (compensation gain) K2, when the absolute value of lateral acceleration G y is equal to or greater than the second threshold value (for example, equal to or greater than 0.5G), stabilizes the control of the compensation gain K2 Constant value. By doing so, the estimation accuracy of the side slip angle β is improved.

タイヤスリップ角演算部43は、操舵角センサ1が検出した操舵角(タイヤ舵角δ)、ヨーレイトセンサ2が検出したヨーレイトγ、車体速度演算部41が算出した車体速度V、及び車体スリップ角推定部42が算出した車両の横滑り角(車両のスリップ角)βを基に、下記(5)式に従って前後輪それぞれのスリップ角β,β(車輪のスリップ角βt)を算出する。 The tire slip angle calculation unit 43 estimates the steering angle (tire steering angle δ) detected by the steering angle sensor 1, the yaw rate γ detected by the yaw rate sensor 2, the vehicle speed V calculated by the vehicle speed calculation unit 41, and the vehicle slip angle estimation. Based on the vehicle side slip angle (vehicle slip angle) β calculated by the unit 42, the slip angles β f and β r (wheel slip angle βt) of the front and rear wheels are calculated according to the following equation (5).

Figure 2010195327
Figure 2010195327

タイヤスリップ角演算部43は、算出したスリップ角βt(β),βt(β)を路面μ推定値演算部45に出力する。
スリップ率演算部44は、車輪速センサ5が検出した各車輪11FL〜11RRの車輪速及び車体速度演算部41が算出した車体速度を基に、前後輪(前輪2輪分と後輪2輪分)のスリップ率λ,λを算出する。スリップ率演算部44は、算出した結果をスリップ率λ,λを路面μ推定値演算部45に出力する。
Tire slip angle calculating section 43 outputs the calculated slip angle βt f f), and outputs [beta] t r a (beta r) of the road surface μ estimated value calculating section 45.
The slip ratio calculating unit 44 is based on the wheel speeds of the respective wheels 11 FL to 11 RR detected by the wheel speed sensor 5 and the vehicle body speed calculated by the vehicle body speed calculating unit 41 (front wheels 2 and rear wheels 2). The slip ratios λ f and λ r of the ring segments are calculated. The slip ratio calculation unit 44 outputs the calculated slip ratios λ f and λ r to the road surface μ estimated value calculation unit 45.

タイヤ力センサ46は、前輪11FL,11FR及び後輪11RL,11RRのタイヤ力を検出する。タイヤ力は、路面からタイヤに作用する力である。すなわちタイヤ力はタイヤから車両に入力される力でもある。具体的には、タイヤ力センサ46は、タイヤ力としてその大きさ及び方向を示すタイヤ力ベクトルを検出する。本実施形態でいうタイヤ力ベクトルは、タイヤと路面間に発生する接地面に平行な力、すなわち制駆動力及び横力を成分とするベクトルである。よって、本実施形態でいうタイヤ力ベクトルには、路面に対して垂直な方向でタイヤに作用する力を含まない。例えば、タイヤ力センサ46は6軸力センサである。また、タイヤ力センサ46を各輪11FL〜11RRに備える。 The tire force sensor 46 detects the tire forces of the front wheels 11 FL and 11 FR and the rear wheels 11 RL and 11 RR . The tire force is a force acting on the tire from the road surface. That is, the tire force is also a force input from the tire to the vehicle. Specifically, the tire force sensor 46 detects a tire force vector indicating the magnitude and direction of the tire force. The tire force vector referred to in the present embodiment is a vector having a force parallel to the contact surface generated between the tire and the road surface, that is, a braking / driving force and a lateral force as components. Therefore, the tire force vector referred to in the present embodiment does not include a force acting on the tire in a direction perpendicular to the road surface. For example, the tire force sensor 46 is a six-axis force sensor. Also includes a tire force sensor 46 to the respective wheels 11 FL to 11 RR.

タイヤ力センサ46は、検出した前後輪のタイヤ力F,Fを路面μ推定値演算部45に出力する。本実施形態のように各輪11FL〜11RRにタイヤ力センサ46を備える場合には、タイヤ力センサ46は、前左右輪の平均値を前輪のタイヤ力Fとして出力し、後左右輪の平均値を後輪のタイヤ力Fとして出力する。
路面μ推定値演算部45は、タイヤスリップ角演算部43が算出した前後輪のスリップ角βt,βt、スリップ率演算部44が算出した前後輪のスリップ率λ,λ、及びタイヤ力センサ46が検出した前後輪のタイヤ力F,Fを基に、路面μを推定する。
The tire force sensor 46 outputs the detected tire forces F f and F r of the front and rear wheels to the road surface μ estimated value calculation unit 45. When each wheel 11 FL to 11 RR includes the tire force sensor 46 as in the present embodiment, the tire force sensor 46 outputs the average value of the front left and right wheels as the tire force F f of the front wheel, and the rear left and right wheels. Is output as the tire force F r of the rear wheel.
Road μ estimated value calculating section 45, the slip angle [beta] t f of the front and rear wheels of tire slip angle calculating section 43 is calculated, [beta] t r, the slip ratio of the front and rear wheels slip rate calculating section 44 has calculated lambda f, lambda r, and the tire The road surface μ is estimated based on the tire forces F f and F r of the front and rear wheels detected by the force sensor 46.

そのため、路面μ推定値演算部45は、図36(a)に示すように、前記図22に示した3次元曲面を3D特性マップ45aとして有する。なお、図36(a)では、3D特性マップ45aを表すものとして、スリップ度と車輪力との関係を表す3次元曲面を1/4周分(1/4象限)強しか表示していない。しかし、実際には、3D特性マップ45aでは、スリップ度と車輪力との関係を表す3次元曲面が全周分存在しており、3D特性マップ45aはドーム状又は半球状になる。タイヤグリップ状態演算部48は、このような3D特性マップ45aを前後輪それぞれに対応させて有する。例えば、メモリ等の記憶媒体に3D特性マップ45aを記憶し、保持している。   Therefore, the road surface μ estimated value calculation unit 45 includes the three-dimensional curved surface shown in FIG. 22 as a 3D characteristic map 45a as shown in FIG. In FIG. 36 (a), as a representation of the 3D characteristic map 45a, a three-dimensional curved surface representing the relationship between the slip degree and the wheel force is displayed only for 1/4 turn (1/4 quadrant). However, in practice, in the 3D characteristic map 45a, a three-dimensional curved surface representing the relationship between the slip degree and the wheel force exists for the entire circumference, and the 3D characteristic map 45a is dome-shaped or hemispherical. The tire grip state calculation unit 48 has such a 3D characteristic map 45a corresponding to each of the front and rear wheels. For example, the 3D characteristic map 45a is stored and held in a storage medium such as a memory.

この3D特性マップ45aは、制駆動力Fx軸とスリップ度Z軸とを含む平面内では、図36(b)に示すように、制駆動力Fxとスリップ度Z(スリップ率λ)との相関関係を示すタイヤ特性曲線を示す。また、3D特性マップ45aは、横力Fy軸とスリップ度Z軸とを含む平面内では、図36(c)に示すように、横力Fyとスリップ度Z(スリップ角βt)との相関関係を示すタイヤ特性曲線を示す。また、3D特性マップ45aは、合力Fとスリップ度Z軸とを含む平面内では、図36(d)に示すように、合力Fとスリップ度Z(スリップ率λとスリップ角βtとの合成値)との相関関係を示すタイヤ特性曲線を示す。   This 3D characteristic map 45a shows a correlation between the braking / driving force Fx and the slip degree Z (slip rate λ) as shown in FIG. 36 (b) in a plane including the braking / driving force Fx axis and the slip degree Z axis. The tire characteristic curve which shows a relationship is shown. Further, in the 3D characteristic map 45a, the correlation between the lateral force Fy and the slip degree Z (slip angle βt) is shown in FIG. 36C in a plane including the lateral force Fy axis and the slip degree Z axis. The tire characteristic curve which shows is shown. Further, as shown in FIG. 36 (d), the 3D characteristic map 45a is a composite value of the resultant force F and the slip degree Z (slip ratio λ and slip angle βt within a plane including the resultant force F and the slip degree Z axis. The tire characteristic curve which shows a correlation with this is shown.

ここで、ある基準路面にて事前に直進走行試験と旋回走行実験とを行い、そのときのデータを基に、このような3D特性マップを作成する。具体的には、基準路面にて実車での直進加加速実験により、制駆動力−スリップ率特性曲線の実計測を行う。さらに、基準路面にて実車での旋回実験(旋回半径一定の加速円旋回が良い)により、横力(コーナリングフォース)−タイヤスリップ角特性曲線の実計測を行う。その実計測結果を基に、3D特性マップを作成する。   Here, a straight running test and a turning test are performed in advance on a certain reference road surface, and such a 3D characteristic map is created based on the data at that time. Specifically, an actual measurement of the braking / driving force-slip ratio characteristic curve is performed by a linear acceleration / acceleration experiment on an actual vehicle on the reference road surface. Further, actual measurement of a lateral force (cornering force) -tire slip angle characteristic curve is performed by a turning test using an actual vehicle on a reference road surface (accelerated circular turning with a constant turning radius is preferable). A 3D characteristic map is created based on the actual measurement result.

また、直接計測ができない場合は、他の物理量を計測しておいて換算することもできる。また、走行実験ではなくシミュレーション等による演算により3D特性マップを得ることもできる。
路面μ推定値演算部45は、以上のような3D特性マップ45aを参照して路面μを推定する。図37は、3D特性マップ45aを参照して路面μを得る関係を、3D特性マップ45aに対する入力と出力との関係として示す。
When direct measurement is not possible, other physical quantities can be measured and converted. Further, it is possible to obtain a 3D characteristic map not by a driving experiment but by calculation by simulation or the like.
The road surface μ estimated value calculation unit 45 estimates the road surface μ with reference to the 3D characteristic map 45a as described above. FIG. 37 shows a relationship for obtaining the road surface μ with reference to the 3D characteristic map 45a as a relationship between an input and an output with respect to the 3D characteristic map 45a.

先ず前輪の場合について説明すると、図37に示すように、路面μ推定値演算部45は、前輪のタイヤ力ベクトルFとスリップ度Z(Z)とを入力とする。
このとき、路面μ推定値演算部45は、前輪のスリップ率λとスリップ角βtとを合成し変換してスリップ度Zを得ている。具体的には、路面μ推定値演算部45は、下記(6)式によりスリップ度Zを算出している。
Z=S/SPeak=√((λ/λPeak+(βt/βtPeak) ・・・(6)
First, the case of the front wheel will be described. As shown in FIG. 37, the road surface μ estimated value calculation unit 45 receives the front wheel tire force vector F f and the slip degree Z (Z f ) as inputs.
At this time, the road surface μ estimated value calculation unit 45 obtains the slip degree Z by combining and converting the slip ratio λ f and the slip angle βt f of the front wheels. Specifically, the road surface μ estimated value calculation unit 45 calculates the slip degree Z by the following equation (6).
Z = S / S Peak = √ ((λ / λ Peak ) 2 + (βt / βt Peak ) 2 ) (6)

ここで、λPeakは、基準路面で制駆動力Fx(Fx)が飽和するスリップ率λ(λ)である。βtPeakは、基準路面で横力Fy(Fy)が飽和するスリップ角βt(βt)である。基準路面がドライ路面(μ=1)であれば、λPeak、βtPeakは、ドライ路面に対応する値になる。また、S/SPeakは、スリップ率λの正規化値(λ/λPeak)とスリップ角βtの正規化値(βt/βtPeak)との合成値となる。或いは、S/SPeakは、スリップ率λの正規化値(λ/λPeak)及びスリップ角βtの正規化値(βt/βtPeak)を成分とする値である。 Here, λ Peak is a slip ratio λ (λ f ) at which the braking / driving force Fx (Fx f ) is saturated on the reference road surface. βt Peak is a slip angle βt (βt f ) at which the lateral force Fy (Fy f ) is saturated on the reference road surface. If the reference road surface is a dry road surface (μ = 1), λ Peak and βt Peak are values corresponding to the dry road surface. S / S Peak is a composite value of the normalized value of the slip ratio λ (λ / λ Peak ) and the normalized value of the slip angle βt (βt / βt Peak ). Alternatively, S / S Peak is a value having a normalized value of the slip ratio λ (λ / λ Peak ) and a normalized value of the slip angle βt (βt / βt Peak ) as components.

このスリップ度Zは、本来次元の異なるスリップ率とスリップ角とを同一次元にしつつ、スリップ率及びスリップ角を同時に評価する値である。
そして、路面μ推定値演算部45は、前輪に対応する3D特性マップ45aを参照して、前輪のタイヤ力ベクトルFとスリップ度Zを基に、路面μを算出する。具体的には、路面μ推定値演算部45は、前記図27に示す演算手順に従い、路面μを算出する。
The slip degree Z is a value for evaluating the slip ratio and the slip angle at the same time while making the slip ratio and the slip angle having different dimensions the same dimension.
Then, the road surface μ estimated value calculation unit 45 refers to the 3D characteristic map 45a corresponding to the front wheel, and calculates the road surface μ based on the tire force vector F f of the front wheel and the slip degree Z. Specifically, the road surface μ estimated value calculation unit 45 calculates the road surface μ according to the calculation procedure shown in FIG.

すなわち、路面μ推定値演算部45は、3D特性マップ45aの原点(0,0)と実測点(Zb,Fb)とを通る直線が、その3D特性マップ45aと交わる点の値(Za,Fa)を特定する(前記ステップS23)。
ここで、実測点(Zb,Fb)は、3D特性マップ45aが示されるFx−Fy−Z空間においてスリップ度Zb(実測のスリップ度Z)とタイヤ力ベクトルFb(F)とで特定される座標(プロット点)である。すなわち、Fx−Fy平面上でタイヤ力ベクトルFbにより特定し、Z軸方向をスリップ度Zbで特定できる座標である。
That is, the road surface μ estimated value calculation unit 45 calculates the values (Za, Fa of the points where a straight line passing through the origin (0, 0) and the actual measurement point (Zb, Fb) of the 3D characteristic map 45a intersects the 3D characteristic map 45a. ) Is specified (step S23).
Here, the actual measurement points (Zb, Fb) are specified by the slip degree Zb (actual slip degree Z) and the tire force vector Fb (F f ) in the Fx-Fy-Z space where the 3D characteristic map 45a is shown. Coordinates (plot points). That is, the coordinates can be specified by the tire force vector Fb on the Fx-Fy plane and the Z-axis direction can be specified by the slip degree Zb.

そして、路面μ推定値演算部45は、実測点を得ている現在の走行路面の路面μの算出する(前記ステップS24)。
すなわち、先ず、路面μ推定値演算部45は、前記実測点(Zb,Fb)と3D特性マップ45aの原点とを結ぶ直線の線長b(=√(Zb+Fb))を得る。つまり、車輪の制駆動力、車輪の横力及び車輪のスリップ度を座標軸とする3次元空間における、該制動力、横力及びスリップ度が零である原点から、現在の検出タイヤ力Fの方向でかつ現在の検出スリップ度Zまで延びる直線に該現在のタイヤ力Fの大きさを投影して得た距離bを得る。
Then, the road surface μ estimated value calculation unit 45 calculates the road surface μ of the current traveling road surface from which the actual measurement points are obtained (step S24).
That is, first, the road surface μ estimated value calculation unit 45 obtains a straight line length b (= √ (Zb 2 + Fb 2 )) connecting the actual measurement point (Zb, Fb) and the origin of the 3D characteristic map 45a. That is, from the origin where the braking force, lateral force and slip degree are zero in a three-dimensional space having the wheel braking / driving force, wheel lateral force and wheel slip degree as coordinate axes, the current detected tire force F f A distance b obtained by projecting the magnitude of the current tire force F f onto a straight line extending in the direction and up to the current detected slip degree Z is obtained.

また、先に特定した3D特性マップ45aとの交点の値(Za,Fa)と該3D特性マップ45aの原点とを結ぶ直線の線長a(=√(Za+Fa))を得る。すなわち、前記距離bを得た直線を延長して3D特性マップ45aと交じわる交点と原点との間の距離aを得る。
さらに、線長bと線長aとの比(b/a)を算出する。そして、路面μ推定値演算部45は、その算出した比(b/a)と、3D特性マップ45aを得た路面の路面μ値μとを乗算し、その乗算値を現在の走行路面の路面μ値μとして得る(μ=μ・b/a)。
In addition, a straight line length a (= √ (Za 2 + Fa 2 )) connecting the value (Za, Fa) of the intersection with the previously specified 3D characteristic map 45a and the origin of the 3D characteristic map 45a is obtained. That is, the straight line obtained from the distance b is extended to obtain the distance a between the intersection point intersecting the 3D characteristic map 45a and the origin.
Further, the ratio (b / a) between the line length b and the line length a is calculated. Then, the road surface μ estimated value calculation unit 45 multiplies the calculated ratio (b / a) by the road surface μ value μ A of the road surface from which the 3D characteristic map 45a is obtained, and multiplies the multiplication value of the current traveling road surface. The road surface μ value is obtained as μ BB = μ A · b / a).

以上のような手順により、路面μ推定値演算部45は、前輪の制駆動力Fx、横力Fy及びスリップ度Z(Z)を基に、前輪についての現在の走行路面の路面μを得る。そして、路面μ推定値演算部45は、同様な手順により、後輪のタイヤ力ベクトルF及びスリップ度Z(Z)を基に、後輪について現在の走行路面の路面μを得る。 Through the above procedure, the road surface μ estimated value calculation unit 45 is based on the braking / driving force Fx f , lateral force Fy f and slip degree Z (Z f ) of the front wheels, and the road surface μ of the current traveling road surface for the front wheels. Get. Then, the road surface μ estimated value calculation unit 45 obtains the road surface μ of the current traveling road surface for the rear wheels based on the tire force vector F r and the slip degree Z (Z r ) of the rear wheels by a similar procedure.

(動作)
図38を用いて説明する。
先ず、車体走行状態推定装置8では、車体速度演算部41が車体速度を算出する(ステップS31)。車体走行状態推定装置8では、スリップ率演算部44がその車体速度を基に、前後輪それぞれのスリップ率λ,λを算出する(ステップS32)。さらに、車体走行状態推定装置8では、タイヤスリップ角演算部43が前後輪それぞれのスリップ角βt,βtを算出する(ステップS33)。一方、タイヤ力センサ46が前後輪のタイヤ力ベクトルF,Fを検出する(ステップS34)。
(Operation)
This will be described with reference to FIG.
First, in the vehicle body travel state estimation device 8, the vehicle body speed calculation unit 41 calculates the vehicle body speed (step S31). In the vehicle body running state estimation device 8, the slip ratio calculation unit 44 calculates the slip ratios λ f and λ r for the front and rear wheels based on the vehicle body speed (step S32). Furthermore, the vehicle body travel state estimating device 8, the tire slip angle calculating section 43 of the respective front and rear wheels slip angle [beta] t f, to calculate the [beta] t r (step S33). On the other hand, the tire force sensor 46 detects the tire force vectors F f and F r of the front and rear wheels (step S34).

そして、車体走行状態推定装置8では、路面μ推定値演算部45が、前後輪のスリップ率λ,λ、前後輪のスリップ角βt,βt及び前後輪のタイヤ力ベクトルF,Fを基に路面μを推定する。車体走行状態推定装置8は、算出した路面μ推定値をEPSECU6及び制駆動モータECU22に出力する。
EPSECU6は、路面μ推定値を基に、操舵アシスト指令によりEPSモータ7を制御する。具体的には、EPSECU6は、路面μ推定値が小さくなるほど、EPSモータ7の出力を低減される制御を行う。
Then, the vehicle body travel state estimating device 8, the road surface μ estimated value calculating section 45, the slip ratio lambda f of the front and rear wheels, lambda r, slip angle [beta] t f of the front and rear wheels, [beta] t r and the front and rear wheels of the tire force vector F f, The road surface μ is estimated based on F r . The vehicle body travel state estimation device 8 outputs the calculated road surface μ estimated value to the EPS ECU 6 and the braking / driving motor ECU 22.
The EPS ECU 6 controls the EPS motor 7 by a steering assist command based on the estimated road surface μ value. Specifically, the EPS ECU 6 performs control such that the output of the EPS motor 7 is reduced as the estimated road surface μ value decreases.

また、制駆動モータECU22は、路面μ推定値を基に、駆動トルク指令値により制駆動モータ21FL〜21RRを制御する。具体的には、制駆動モータECU22は、路面μ推定値が小さくなるほど駆動トルク指令値を小さくして駆動力の出力を抑制する制御を行う。又は、制駆動モータECU22は、路面μ推定値が小さくなるほど制動トルク指令値を小さくして制動力の出力を抑制する制御を行う。 The braking / driving motor ECU 22 controls the braking / driving motors 21 FL to 21 RR based on the driving torque command value based on the estimated road surface μ value. Specifically, the braking / driving motor ECU 22 performs control to suppress the output of the driving force by decreasing the driving torque command value as the estimated road surface μ value decreases. Alternatively, the braking / driving motor ECU 22 performs control to suppress the output of the braking force by decreasing the braking torque command value as the estimated road surface μ value decreases.

(実施形態の変形例)
(1)この実施形態では、タイヤ特性相関関係マップが、車輪の制駆動力、車輪の横力及び車輪のスリップ度を座標軸とする3次元空間に存在するものとして、連続した3次元曲面として表現された3D特性マップである。これに対して、3D特性マップ(タイヤ特性相関関係マップ)を、車輪の制駆動力、車輪の横力及び車輪のスリップ度を変数として数式表現されたものとすることもできる。
(Modification of the embodiment)
(1) In this embodiment, the tire characteristic correlation map is expressed as a continuous three-dimensional curved surface, assuming that the tire characteristic correlation map exists in a three-dimensional space having the wheel braking / driving force, wheel lateral force, and wheel slip degree as coordinate axes. 3D characteristic map obtained. On the other hand, the 3D characteristic map (tire characteristic correlation map) may be expressed numerically with the braking / driving force of the wheel, the lateral force of the wheel, and the slip degree of the wheel as variables.

(2)この実施形態では、3D特性マップを得る基準路面として乾燥アスファルトといったようなドライ路面を想定して、その路面μ値をμ=1.0にしている。しかし、これに限定されるものではない。例えば、潤湿路面や凍結路面を基準路面として3D特性マップを作成することもできる。なお、基準路面を高路面μとすれば、計器ノイズ等の外乱を相対的に抑えることができるといった利点がある。 (2) In this embodiment, a dry road surface such as dry asphalt is assumed as a reference road surface for obtaining a 3D characteristic map, and the road surface μ value is set to μ = 1.0. However, it is not limited to this. For example, a 3D characteristic map can be created using a wet road surface or a frozen road surface as a reference road surface. If the reference road surface is a high road surface μ, there is an advantage that disturbances such as instrument noise can be relatively suppressed.

(3)この実施形態では、制駆動力Fx及び横力Fyを同時に様々な方向に振って、すなわち、合力の方向を様々に振って、3D特性マップを得ている。これに対して、前後方向(制駆動力Fx)の2Dの特性マップと横方向(横力Fy)の2Dのμ特性マップとを別々に得て、それら2D特性マップ間を補完して3D特性マップを得ることもできる。この場合、2D特性マップ間を楕円近似して補完する。 (3) In this embodiment, the braking / driving force Fx and the lateral force Fy are simultaneously swung in various directions, that is, the direction of the resultant force is swung in various directions to obtain a 3D characteristic map. On the other hand, a 2D characteristic map in the front-rear direction (braking / driving force Fx) and a 2D μ characteristic map in the lateral direction (lateral force Fy) are obtained separately, and the 3D characteristics are complemented between these 2D characteristic maps. You can also get a map. In this case, the 2D characteristic maps are complemented by elliptical approximation.

(4)この実施形態では、操舵制御(操舵反力付加制御)により車両の旋回挙動又は横方向挙動を制御している。これに対して、VDC(Vehicle DynamicsControl)等の左右輪の制駆動力差による旋回制御により車両挙動を制御することもできる。これにより、さらに応答性の速い車両挙動安定化制御(横滑り防止制御)を実現することができる。
(5)この実施形態では、前輪操舵車両を例に挙げている。これに対して、後輪操舵車両とすることもできる。
(4) In this embodiment, the turning behavior or lateral behavior of the vehicle is controlled by steering control (steering reaction force addition control). On the other hand, the vehicle behavior can also be controlled by turning control based on the braking / driving force difference between the left and right wheels such as VDC (Vehicle Dynamics Control). As a result, it is possible to realize vehicle behavior stabilization control (side slip prevention control) with even faster response.
(5) In this embodiment, a front wheel steering vehicle is taken as an example. On the other hand, it can also be set as a rear-wheel steering vehicle.

(6)この実施形態では、前後輪それぞれについて路面μを算出している。これに対して、左右輪それぞれ(4輪別々)について路面μを算出することもできる。また、全輪について、ある一つの路面μを算出することもできる。
(7)この実施形態では、路面μを基に操舵制御するEPSECU6と、路面μを基に制駆動力制御する制駆動モータECU22とを備えている。これに対して、EPSECU6及び制駆動モータECU22の何れか一方だけを備えることもできる。すなわち、路面μを基に、制駆動力制御及び操舵制御の何れか一方だけを実施することもできる。
(6) In this embodiment, the road surface μ is calculated for each of the front and rear wheels. On the other hand, the road surface μ can be calculated for each of the left and right wheels (separately for four wheels). It is also possible to calculate a certain road surface μ for all the wheels.
(7) This embodiment includes an EPS ECU 6 that performs steering control based on the road surface μ, and a braking / driving motor ECU 22 that performs braking / driving force control based on the road surface μ. On the other hand, only one of EPSECU 6 and braking / driving motor ECU 22 can be provided. That is, only one of braking / driving force control and steering control can be performed based on the road surface μ.

なお、この実施形態では、車両の車輪の接地面グリップ特性を推定するための車両接地面摩擦状態推定装置を実現する。また、タイヤ力センサ46は、車輪の制駆動力及び横力を成分に含む車輪のタイヤ力の方向及び大きさを検出するタイヤ力検出手段を実現する。また、タイヤスリップ角演算部43及びスリップ率演算部44は、前記車輪のスリップ度を検出するスリップ度検出手段を実現する。また、路面μ推定値演算部47及び3D特性マップ47aは、基準路面摩擦係数の基準路面で得られる車輪の制駆動力、車輪の横力及び車輪のスリップ度の相関関係で成立する3次元曲面を表すタイヤ特性をモデル化したタイヤ特性相関関係マップを実現する。また、路面μ推定値演算部47は、前記タイヤ力検出手段が検出した現在のタイヤ力、前記スリップ度検出手段が検出した現在のスリップ度及びタイヤ特性相関関係マップを基に、現在の路面の路面摩擦係数を算出する路面摩擦係数算出手段を実現する。   In this embodiment, a vehicle ground contact surface friction state estimation device for estimating the ground contact surface grip characteristics of the vehicle wheel is realized. Further, the tire force sensor 46 realizes tire force detection means for detecting the direction and magnitude of the wheel tire force including the braking / driving force and lateral force of the wheel as components. Further, the tire slip angle calculation unit 43 and the slip ratio calculation unit 44 realize a slip degree detection means for detecting the slip degree of the wheel. Further, the road surface μ estimated value calculation unit 47 and the 3D characteristic map 47a are a three-dimensional curved surface formed by the correlation between the braking / driving force of the wheel, the lateral force of the wheel, and the slip degree of the wheel obtained on the reference road surface of the reference road surface friction coefficient. The tire characteristic correlation map that models the tire characteristic that represents is realized. Further, the road surface μ estimated value calculating unit 47 calculates the current road surface based on the current tire force detected by the tire force detecting unit, the current slip degree detected by the slip degree detecting unit, and the tire characteristic correlation map. A road surface friction coefficient calculating means for calculating a road surface friction coefficient is realized.

また、この実施形態では、前記タイヤ特性相関関係マップは、前記基準路面での制駆動力と横力との合力とスリップ度との比と基準路面摩擦係数とは異なる路面摩擦係数の路面での制駆動力と横力との合力とスリップ度との比が同一であれば、前記基準路面での制駆動力と横力との合力と、基準路面摩擦係数とは異なる路面摩擦係数の路面での制駆動力と横力との合力との比、又は前記基準路面でのスリップ度と、基準路面摩擦係数とは異なる路面摩擦係数の路面でのスリップ度との比が、基準路面摩擦係数と、基準路面摩擦係数とは異なる路面摩擦係数との比を示す特性を有している。
ここで、基準路面摩擦係数とは異なる路面摩擦係数とは、基準路面摩擦係数以外の任意の路面摩擦係数である。
Further, in this embodiment, the tire characteristic correlation map is obtained on the road surface having a road surface friction coefficient different from a ratio of a resultant force of the braking / driving force and lateral force on the reference road surface and a slip ratio and a reference road surface friction coefficient. If the ratio of the resultant force of the braking / driving force and the lateral force and the slip ratio is the same, the resultant force of the braking / driving force and the lateral force on the reference road surface is different from the reference road surface friction coefficient on the road surface. The ratio between the braking / driving force and the resultant force of the lateral force, or the ratio of the slip degree on the reference road surface and the slip degree on the road surface having a road surface friction coefficient different from the reference road surface friction coefficient is the reference road surface friction coefficient. In addition, it has a characteristic indicating a ratio of a road surface friction coefficient different from the reference road surface friction coefficient.
Here, the road surface friction coefficient different from the reference road surface friction coefficient is an arbitrary road surface friction coefficient other than the reference road surface friction coefficient.

また、この実施形態では、前記路面摩擦係数算出手段は、前記車輪の制駆動力、車輪の横力及び車輪のスリップ度を座標軸とする3次元空間における、該制動力、横力及びスリップ度が零である原点から前記タイヤ力ベクトル検出手段が検出した現在のタイヤ力の方向でかつ前記スリップ度検出手段が検出した現在のスリップ度まで延びる直線に該現在のタイヤ力の大きさを投影して得た距離と、前記直線を延長して前記タイヤ特性相関関係マップと交じわる交点と前記原点との間の距離との比を基に、現在の路面の路面摩擦係数を算出する。   Further, in this embodiment, the road surface friction coefficient calculating means has the braking force, lateral force, and slip degree in a three-dimensional space having the wheel braking / driving force, wheel lateral force, and wheel slip degree as coordinate axes. Projecting the magnitude of the current tire force onto a straight line extending from the zero origin to the current tire force direction detected by the tire force vector detecting means and to the current slip degree detected by the slip degree detecting means. The road surface friction coefficient of the current road surface is calculated based on the ratio between the obtained distance and the distance between the intersection and the origin that extends the straight line and intersects the tire characteristic correlation map.

また、この実施形態では、車両の車輪の接地面グリップ特性を推定するための車両接地面摩擦状態推定方法において、車輪の制駆動力及び横力を成分に含む車輪のタイヤ力のベクトル及び車輪のスリップ度を検出する検出ステップと、前記検出ステップで検出した現在のタイヤ力ベクトル、現在のスリップ度及びタイヤ特性相関関係マップを基に、現在の路面の路面摩擦係数を算出する路面摩擦係数算出ステップと、を有し、前記タイヤ特性相関関係マップは、基準路面摩擦係数の基準路面で得られる車輪の制駆動力、車輪の横力及び車輪のスリップ度の相関関係で成立する3次元曲面を表すタイヤ特性をモデル化したものであり、前記基準路面での制駆動力と横力との合力とスリップ度との比と基準路面摩擦係数とは異なる路面摩擦係数の路面での制駆動力と横力との合力とスリップ度との比が同一であれば、前記基準路面での制駆動力と横力との合力と、基準路面摩擦係数とは異なる路面摩擦係数の路面での制駆動力と横力との合力との比、又は前記基準路面でのスリップ度と、基準路面摩擦係数とは異なる路面摩擦係数の路面でのスリップ度との比が、基準路面摩擦係数と、基準路面摩擦係数とは異なる路面摩擦係数との比を示す特性を有し、前記路面摩擦係数算出ステップは、前記車輪の制駆動力、車輪の横力及び車輪のスリップ度を座標軸とする3次元空間における、該制動力、横力及びスリップ度が零である原点から前記検出ステップで検出した現在のタイヤ力の方向でかつ前記検出ステップで検出した現在のスリップ度まで延びる直線に該現在のタイヤ力の大きさを投影して得た距離と、前記直線を延長して前記タイヤ特性相関関係マップと交じわる交点と前記原点との間の距離との比を基に、現在の路面の路面摩擦係数を算出する車両接地面摩擦状態推定方法を実現する。   Further, in this embodiment, in the vehicle ground contact surface friction state estimation method for estimating the ground contact surface grip characteristic of the vehicle wheel, the wheel tire force vector including the wheel braking / driving force and lateral force as components, and the wheel Detection step for detecting the slip degree, and a road surface friction coefficient calculating step for calculating the road surface friction coefficient of the current road surface based on the current tire force vector detected in the detection step, the current slip degree and the tire characteristic correlation map The tire characteristic correlation map represents a three-dimensional curved surface established by the correlation of the braking / driving force of the wheel, the lateral force of the wheel and the slip degree of the wheel obtained on the reference road surface of the reference road surface friction coefficient. The tire characteristics are modeled, and the ratio of the resultant friction between the braking / driving force and lateral force on the reference road surface and the slip ratio is different from the reference road surface friction coefficient. If the ratio of the resultant force between the braking / driving force and the lateral force on the surface and the slip ratio is the same, the resultant force of the braking / driving force and the lateral force on the reference road surface is different from the reference road friction coefficient. The ratio of the resultant force of braking / driving force and lateral force on the road surface, or the ratio of the slip degree on the reference road surface to the slip degree on the road surface having a road surface friction coefficient different from the reference road surface friction coefficient is the reference road surface. The road surface friction coefficient calculation step has a characteristic indicating a ratio between a friction coefficient and a road surface friction coefficient different from a reference road surface friction coefficient, and the road surface friction coefficient calculation step uses coordinate axes of the braking / driving force of the wheel, the lateral force of the wheel, and the slip degree of the wheel. In a three-dimensional space, a straight line extending from the origin where the braking force, lateral force and slip degree are zero to the current tire force direction detected in the detection step and to the current slip degree detected in the detection step. The size of the current tire force The road surface friction coefficient of the current road surface is calculated based on the ratio between the distance obtained by the shadow and the distance between the intersection and the origin of the tire characteristic correlation map by extending the straight line. A vehicle ground contact surface friction state estimation method is realized.

(実施形態の効果)
(1)基準路面摩擦係数の基準路面での制駆動力と横力との合力とスリップ度との比と基準路面摩擦係数とは異なる路面摩擦係数の路面での制駆動力と横力との合力とスリップ度との比が同一であれば、基準路面での制駆動力と横力との合力と、基準路面摩擦係数とは異なる路面摩擦係数の路面での制駆動力と横力との合力との比、又は基準路面でのスリップ度と、基準路面摩擦係数とは異なる路面摩擦係数の路面でのスリップ度との比が、基準路面摩擦係数とこの基準路面摩擦係数とは異なる路面摩擦係数との比を示す特性を有する。
(Effect of embodiment)
(1) The ratio of the resultant force of the braking / driving force and the lateral force on the reference road surface to the slip degree and the reference road surface friction coefficient is different from the reference road surface friction coefficient. If the ratio of the resultant force and the slip ratio is the same, the resultant force between the braking / driving force and the lateral force on the reference road surface and the braking / driving force and the lateral force on the road surface with a road surface friction coefficient different from the reference road surface friction coefficient are calculated. The ratio of the resultant force or the slip ratio on the reference road surface to the slip ratio on the road surface having a different road friction coefficient from the reference road friction coefficient is different from the reference road friction coefficient and the reference road friction coefficient. It has a characteristic indicating a ratio with a coefficient.

そして、車輪の制駆動力、車輪の横力及び車輪のスリップ度を座標軸とする3次元空間でみると、基準路面での制駆動力と横力との合力とスリップ度との比と基準路面摩擦係数とは異なる路面摩擦係数の路面での制駆動力と横力との合力とスリップ度との比が同一であるときに、基準路面での制駆動力と横力との合力と、基準路面摩擦係数とは異なる路面摩擦係数の路面での制駆動力と横力との合力との比、又は基準路面でのスリップ度と、基準路面摩擦係数とは異なる路面摩擦係数の路面でのスリップ度との比と、3次元空間の原点から検出した現在のタイヤ力の方向でかつ検出した現在のスリップ度まで延びる直線に該現在のタイヤ力の大きさを投影して得た距離と、前記直線を延長してタイヤ特性相関関係マップと交じわる交点と前記原点との間の距離との比とは、幾何学的にみて一致する。   Then, when viewed in a three-dimensional space with the wheel braking / driving force, wheel lateral force and wheel slip degree as coordinate axes, the ratio of the resultant force of the braking / driving force and lateral force on the reference road surface to the slip degree and the reference road surface When the ratio of the resultant force between the braking / driving force and the lateral force on the road surface having a different friction coefficient from the friction coefficient and the slip ratio is the same, the resultant force between the braking / driving force and the lateral force on the reference road surface and the reference The ratio of the resultant force of braking / driving force and lateral force on the road surface with a road surface friction coefficient different from the road surface friction coefficient, or the slip degree on the reference road surface, and the slip on the road surface with a road surface friction coefficient different from the reference road surface friction coefficient The distance obtained by projecting the magnitude of the current tire force on a straight line extending in the direction of the current tire force detected from the origin of the three-dimensional space and extending to the detected current slip degree; An intersection that extends a straight line and intersects with the tire characteristic correlation map The ratio of the distance between the points, match viewed geometrically.

よって、3次元空間の原点から検出した現在のタイヤ力の方向でかつ検出した現在のスリップ度まで延びる直線に該現在のタイヤ力の大きさを投影して得た距離と、前記直線を延長してタイヤ特性相関関係マップと交じわる交点と前記原点との間の距離との比、及び基準路面摩擦係数から、現在の路面の路面摩擦係数を算出できる。
これにより、車輪のタイヤ力の方向と大きさ、及びスリップ度を検出して、現在の路面の路面摩擦係数を算出できる。
この結果、スリップが発生する前に現在の路面の路面摩擦係数を推定できる。
Therefore, the distance obtained by projecting the magnitude of the current tire force on a straight line extending from the origin of the three-dimensional space to the detected current slip degree in the direction of the current tire force, and the straight line is extended. Thus, the road surface friction coefficient of the current road surface can be calculated from the ratio of the intersection between the tire characteristic correlation map and the distance between the origin and the reference road surface friction coefficient.
Thereby, the direction and magnitude | size of the tire force of a wheel and a slip degree are detected, and the road surface friction coefficient of the present road surface is computable.
As a result, the road surface friction coefficient of the current road surface can be estimated before slip occurs.

(2)タイヤ力検出手段は、タイヤ力のベクトルを検出する。
これにより、タイヤ力の方向と大きさを同時に検出できる。
(3)タイヤ特性相関関係マップは、車輪の制駆動力、車輪の横力及び車輪のスリップ度を座標軸とする3次元空間に存在するものとして、連続した3次元曲面として表現されたものである。
これにより、高い精度でかつ簡単に現在の路面の路面摩擦係数を推定できる。
(2) The tire force detecting means detects a tire force vector.
Thereby, the direction and magnitude of the tire force can be detected simultaneously.
(3) The tire characteristic correlation map is expressed as a continuous three-dimensional curved surface as being present in a three-dimensional space having the wheel braking / driving force, wheel lateral force and wheel slip degree as coordinate axes. .
Thereby, the road surface friction coefficient of the current road surface can be easily estimated with high accuracy.

(4)タイヤ特性相関関係マップは、車輪の制駆動力、車輪の横力及び車輪のスリップ度を変数として数式表現されたものである。
これにより、高い精度でかつ簡単に現在の路面の路面摩擦係数を推定できる。
(5)スリップ度は、車輪のスリップ率と車輪のスリップ角とを成分とした値である。
これにより、車輪のスリップ率と車輪のスリップ角とに対応して現在の路面の路面摩擦係数を推定できる。
(6)スリップ度は、車輪のスリップ率及び車輪のスリップ角それぞれの無次元値を合成した値である。
無次元化したことで一般化したスリップ度を基に、現在の路面の路面摩擦係数を推定できる。
(4) The tire characteristic correlation map is expressed mathematically using the braking / driving force of the wheel, the lateral force of the wheel, and the slip degree of the wheel as variables.
Thereby, the road surface friction coefficient of the current road surface can be easily estimated with high accuracy.
(5) The slip degree is a value having the slip ratio of the wheel and the slip angle of the wheel as components.
Thereby, the road surface friction coefficient of the present road surface can be estimated corresponding to the slip ratio of the wheel and the slip angle of the wheel.
(6) The slip degree is a value obtained by combining dimensionless values of the wheel slip ratio and the wheel slip angle.
The road surface friction coefficient of the current road surface can be estimated based on the degree of slip that is generalized by making it dimensionless.

(7)車輪のスリップ率を基準路面で車輪の制駆動力が飽和する車輪のスリップ率で除すことで、車輪のスリップ率の無次元値を得ている。
無次元化したことで一般化したスリップ度を基に、現在の路面の路面摩擦係数を推定できる。
(8)車輪のスリップ角を基準路面で車輪の横力が飽和する車輪のスリップ角で除すことで、車輪のスリップ角の無次元値を得ている。
無次元化したことで一般化したスリップ度を基に、現在の路面の路面摩擦係数を推定できる。
(7) A dimensionless value of the wheel slip ratio is obtained by dividing the wheel slip ratio by the wheel slip ratio at which the braking / driving force of the wheel is saturated on the reference road surface.
The road surface friction coefficient of the current road surface can be estimated based on the degree of slip that is generalized by making it dimensionless.
(8) A dimensionless value of the wheel slip angle is obtained by dividing the wheel slip angle by the wheel slip angle at which the lateral force of the wheel is saturated on the reference road surface.
The road surface friction coefficient of the current road surface can be estimated based on the degree of slip that is generalized by making it dimensionless.

43 タイヤスリップ角演算部、44 スリップ率演算部、45 路面μ推定値演算部、45a 3D特性マップ、46 タイヤ力センサ   43 tire slip angle calculation unit, 44 slip ratio calculation unit, 45 road surface μ estimated value calculation unit, 45a 3D characteristic map, 46 tire force sensor

Claims (9)

車両の車輪の接地面グリップ特性を推定するための車両接地面摩擦状態推定装置において、
車輪の制駆動力及び横力を成分に含む車輪のタイヤ力の方向及び大きさを検出するタイヤ力検出手段と、
前記車輪のスリップ度を検出するスリップ度検出手段と、
基準路面摩擦係数の基準路面で得られる車輪の制駆動力、車輪の横力及び車輪のスリップ度の相関関係で成立する3次元曲面を表すタイヤ特性をモデル化したタイヤ特性相関関係マップと、
前記タイヤ力検出手段が検出した現在のタイヤ力、前記スリップ度検出手段が検出した現在のスリップ度及びタイヤ特性相関関係マップを基に、現在の路面の路面摩擦係数を算出する路面摩擦係数算出手段と、を備え、
前記タイヤ特性相関関係マップは、前記基準路面での制駆動力と横力との合力とスリップ度との比と基準路面摩擦係数とは異なる路面摩擦係数の路面での制駆動力と横力との合力とスリップ度との比が同一であれば、前記基準路面での制駆動力と横力との合力と、基準路面摩擦係数とは異なる路面摩擦係数の路面での制駆動力と横力との合力との比、又は前記基準路面でのスリップ度と、基準路面摩擦係数とは異なる路面摩擦係数の路面でのスリップ度との比が、基準路面摩擦係数と、基準路面摩擦係数とは異なる路面摩擦係数との比を示す特性を有し、
前記路面摩擦係数算出手段は、前記車輪の制駆動力、車輪の横力及び車輪のスリップ度を座標軸とする3次元空間における、該制動力、横力及びスリップ度が零である原点から前記タイヤ力ベクトル検出手段が検出した現在のタイヤ力の方向でかつ前記スリップ度検出手段が検出した現在のスリップ度まで延びる直線に該現在のタイヤ力の大きさを投影して得た距離と、前記直線を延長して前記タイヤ特性相関関係マップと交じわる交点と前記原点との間の距離との比を基に、現在の路面の路面摩擦係数を算出することを特徴とする車両接地面摩擦状態推定装置。
In the vehicle ground contact surface friction state estimation device for estimating the ground contact surface grip characteristics of the vehicle wheel,
Tire force detecting means for detecting the direction and magnitude of the wheel tire force including the braking / driving force and lateral force of the wheel as components;
Slip degree detecting means for detecting the slip degree of the wheel;
A tire characteristic correlation map that models tire characteristics representing a three-dimensional curved surface formed by the correlation of wheel braking / driving force, wheel lateral force, and wheel slip degree obtained on the reference road surface of the reference road surface friction coefficient;
Road surface friction coefficient calculating means for calculating a road surface friction coefficient of the current road surface based on the current tire force detected by the tire force detecting means, the current slip degree detected by the slip degree detecting means, and a tire characteristic correlation map. And comprising
The tire characteristic correlation map includes a ratio of a resultant force between a braking / driving force and a lateral force on the reference road surface and a slip ratio, and a braking / driving force and a lateral force on a road surface having a road surface friction coefficient different from the reference road surface friction coefficient. If the ratio of the resultant force to the slip ratio is the same, the resultant force of the braking / driving force and lateral force on the reference road surface, and the braking / driving force and lateral force on the road surface having a road surface friction coefficient different from the reference road surface friction coefficient The ratio of the slip ratio on the road surface and the ratio of the slip degree on the reference road surface and the slip degree on the road surface having a different road friction coefficient from the reference road surface friction coefficient are the reference road friction coefficient and the reference road surface friction coefficient. It has the characteristic to show the ratio with different road friction coefficient,
The road surface friction coefficient calculating means is configured such that the tire from the origin where the braking force, lateral force, and slip degree are zero in a three-dimensional space with the wheel braking / driving force, wheel lateral force, and wheel slip degree as coordinate axes. A distance obtained by projecting the magnitude of the current tire force on a straight line extending in the direction of the current tire force detected by the force vector detecting means and extending to the current slip degree detected by the slip degree detecting means; The road contact surface friction state is calculated by calculating a road surface friction coefficient of the current road surface based on a ratio of a distance between the intersection point intersecting with the tire characteristic correlation map and the origin point Estimating device.
前記タイヤ力検出手段は、前記タイヤ力のベクトルを検出することを特徴とする請求項1に記載の車両接地面摩擦状態推定装置。   The vehicle tire contact surface friction state estimation device according to claim 1, wherein the tire force detection means detects a vector of the tire force. 前記タイヤ特性相関関係マップは、前記車輪の制駆動力、車輪の横力及び車輪のスリップ度を座標軸とする3次元空間に存在するものとして、連続した3次元曲面として表現されたものであることを特徴とする請求項1又は2に記載の車両接地面摩擦状態推定装置。   The tire characteristic correlation map is expressed as a continuous three-dimensional curved surface as existing in a three-dimensional space having the wheel braking / driving force, wheel lateral force and wheel slip degree as coordinate axes. The vehicle ground contact surface friction state estimation device according to claim 1 or 2. 前記タイヤ特性相関関係マップは、前記車輪の制駆動力、車輪の横力及び車輪のスリップ度を変数として数式表現されたものであることを特徴とする請求項1又は2に記載の車両接地面摩擦状態推定装置。   3. The vehicle ground contact surface according to claim 1, wherein the tire characteristic correlation map is expressed mathematically by using the braking / driving force of the wheel, the lateral force of the wheel, and the slip degree of the wheel as variables. Friction state estimation device. 前記スリップ度は、車輪のスリップ率と車輪のスリップ角とを成分とした値であることを特徴とする請求項1〜4の何れか1項に記載の車両接地面摩擦状態推定装置。   The vehicle slip surface friction state estimation device according to any one of claims 1 to 4, wherein the slip degree is a value that includes a slip ratio of a wheel and a slip angle of the wheel. 前記スリップ度は、車輪のスリップ率及び車輪のスリップ角それぞれの無次元値を成分とした値であることを特徴とする請求項1〜5の何れか1項に記載の車両接地面摩擦状態推定装置。   The vehicle slip surface friction state estimation according to any one of claims 1 to 5, wherein the slip degree is a value having a dimensionless value of each of a wheel slip ratio and a wheel slip angle as a component. apparatus. 前記車輪のスリップ率を前記基準路面で車輪の制駆動力が飽和する車輪のスリップ率で除すことで、前記車輪のスリップ率の無次元値を得ていることを特徴とする請求項6に記載の車両接地面摩擦状態推定装置。   The dimensionless value of the slip ratio of the wheel is obtained by dividing the slip ratio of the wheel by the slip ratio of the wheel at which the braking / driving force of the wheel is saturated on the reference road surface. The vehicle ground contact surface friction state estimation apparatus as described. 前記車輪のスリップ角を前記基準路面で車輪の横力が飽和する車輪のスリップ角で除すことで、前記車輪のスリップ角の無次元値を得ていることを特徴とする請求項6又は7に記載の車両接地面摩擦状態推定装置。   The dimensionless value of the slip angle of the wheel is obtained by dividing the slip angle of the wheel by the slip angle of the wheel at which the lateral force of the wheel is saturated on the reference road surface. Vehicle ground contact surface friction state estimation device according to claim 1. 車両の車輪の接地面グリップ特性を推定するための車両接地面摩擦状態推定方法において、
車輪の制駆動力及び横力を成分に含む車輪のタイヤ力のベクトル及び車輪のスリップ度を検出する検出ステップと、
前記検出ステップで検出した現在のタイヤ力ベクトル、現在のスリップ度及びタイヤ特性相関関係マップを基に、現在の路面の路面摩擦係数を算出する路面摩擦係数算出ステップと、を有し、
前記タイヤ特性相関関係マップは、基準路面摩擦係数の基準路面で得られる車輪の制駆動力、車輪の横力及び車輪のスリップ度の相関関係で成立する3次元曲面を表すタイヤ特性をモデル化したものであり、前記基準路面での制駆動力と横力との合力とスリップ度との比と基準路面摩擦係数とは異なる路面摩擦係数の路面での制駆動力と横力との合力とスリップ度との比が同一であれば、前記基準路面での制駆動力と横力との合力と、基準路面摩擦係数とは異なる路面摩擦係数の路面での制駆動力と横力との合力との比、又は前記基準路面でのスリップ度と、基準路面摩擦係数とは異なる路面摩擦係数の路面でのスリップ度との比が、基準路面摩擦係数と、基準路面摩擦係数とは異なる路面摩擦係数との比を示す特性を有し、
前記路面摩擦係数算出ステップは、前記車輪の制駆動力、車輪の横力及び車輪のスリップ度を座標軸とする3次元空間における、該制動力、横力及びスリップ度が零である原点から前記検出ステップで検出した現在のタイヤ力の方向でかつ前記検出ステップで検出した現在のスリップ度まで延びる直線に該現在のタイヤ力の大きさを投影して得た距離と、前記直線を延長して前記タイヤ特性相関関係マップと交じわる交点と前記原点との間の距離との比を基に、現在の路面の路面摩擦係数を算出することを特徴とする車両接地面摩擦状態推定方法。
In the vehicle ground contact surface friction state estimation method for estimating the ground contact surface grip characteristics of the vehicle wheel,
A detection step of detecting a wheel tire force vector including wheel braking / driving force and lateral force as components and a wheel slip degree;
A road surface friction coefficient calculating step for calculating a road surface friction coefficient of the current road surface based on the current tire force vector detected in the detection step, the current slip degree and the tire characteristic correlation map, and
The tire characteristic correlation map models a tire characteristic representing a three-dimensional curved surface formed by a correlation of wheel braking / driving force, wheel lateral force and wheel slip degree obtained on the reference road surface of the reference road surface friction coefficient. The ratio of the resultant force between the braking / driving force and lateral force on the reference road surface and the slip ratio, and the resultant force of the braking / driving force and the lateral force on the road surface having a road surface friction coefficient different from the reference road friction coefficient and slip If the ratio to the degree is the same, the resultant force of the braking / driving force and the lateral force on the reference road surface and the resultant force of the braking / driving force and the lateral force on the road surface having a road surface friction coefficient different from the reference road surface friction coefficient Or the ratio of the slip degree on the reference road surface to the slip degree on the road surface having a road surface friction coefficient different from the reference road surface friction coefficient is different from the reference road surface friction coefficient and the road surface friction coefficient. And a characteristic indicating the ratio of
The road surface friction coefficient calculating step is performed by detecting the braking force, lateral force and slip degree from a zero point in a three-dimensional space having the wheel braking / driving force, wheel lateral force and wheel slip degree as coordinate axes. A distance obtained by projecting the magnitude of the current tire force on a straight line extending in the direction of the current tire force detected in the step and extending to the current slip degree detected in the detection step; and A vehicle contact surface friction state estimation method, wherein a road surface friction coefficient of a current road surface is calculated based on a ratio between an intersection point intersecting with a tire characteristic correlation map and a distance between the origin.
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