JPH0549943B2 - - Google Patents

Info

Publication number
JPH0549943B2
JPH0549943B2 JP1056090A JP5609089A JPH0549943B2 JP H0549943 B2 JPH0549943 B2 JP H0549943B2 JP 1056090 A JP1056090 A JP 1056090A JP 5609089 A JP5609089 A JP 5609089A JP H0549943 B2 JPH0549943 B2 JP H0549943B2
Authority
JP
Japan
Prior art keywords
road surface
transducer
reflected
pulse width
ultrasonic
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP1056090A
Other languages
Japanese (ja)
Other versions
JPH02236451A (en
Inventor
Chogo Sekine
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Japan Radio Co Ltd
Original Assignee
Japan Radio Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Japan Radio Co Ltd filed Critical Japan Radio Co Ltd
Priority to JP1056090A priority Critical patent/JPH02236451A/en
Publication of JPH02236451A publication Critical patent/JPH02236451A/en
Publication of JPH0549943B2 publication Critical patent/JPH0549943B2/ja
Granted legal-status Critical Current

Links

Description

【発明の詳細な説明】 [産業上の利用分野] この発明は自動車等の車輌(以下、総称して自
動車という)に搭載して走行中に路面の摩擦係数
を検知する路面摩擦係数検知装置に関するもので
ある。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a road surface friction coefficient detection device that is mounted on a vehicle such as an automobile (hereinafter collectively referred to as a vehicle) and detects the friction coefficient of a road surface while driving. It is something.

[従来の技術] 自動車の走行中に急ブレーキを掛けた場合、路
面の状況により車輪がロツクされて横滑りを起こ
す危険性を防止するため、ブレーキの掛かり具合
を電子的に制御するALB(anti lock break)と
呼ばれる横滑り防止装置が広く使われている。
[Prior art] In order to prevent the risk of the wheels locking up and skidding due to road surface conditions when sudden braking is applied while the vehicle is running, anti-lock brakes (ALB) are used to electronically control the degree of brake application. A skid prevention device called ``break'' is widely used.

自動車のブレーキは、ブレーキペダルの踏み圧
に応じた制動力を発揮して車輪を制動し、自動車
の走行スピードを制御して自動車を停止させる働
きをするが、路面が滑り易いと車輪に制動力が働
いても路面上でタイヤが滑つて自動車の走行スビ
ードを巧く制御できなくなる。また、このように
タイヤが滑り出すと、各タイヤそれぞれの制動力
が異なるために自動車が横滑り現象を起こし、事
故が発生する原因になる。この横滑りを防止する
ため横滑り防止装置では、実際に路面上でタイヤ
が滑り出した場合これを検知して、ブレーキペダ
ルの踏み圧のいかんに係わらずタイヤの滑り出し
が停止するまで、車輪の制動力を強制的に制御し
て、このような場合の自動車の横滑りを防止して
いる。
A car's brakes apply braking force to the wheels according to the pressure applied to the brake pedal, controlling the speed of the car and stopping the car. However, if the road surface is slippery, the braking force is applied to the wheels. Even if it works, the tires will slip on the road and the car's speed will not be controlled properly. Furthermore, when the tires start to slip, the braking force of each tire is different, causing the vehicle to skid and causing an accident. In order to prevent this skid, a skid prevention device detects when a tire actually begins to skid on the road surface and applies braking force to the wheel until the tire stops skidding, regardless of the pressure applied to the brake pedal. Forced control is used to prevent the vehicle from skidding in such cases.

[発明が解決しようとする課題] 従来の横滑り防止装置は以上のように構成され
ているので、実際に路面上でタイヤが滑り始めた
後でなければ制御することができず、自動車の横
滑りを防止するという本来の充分な性能が得られ
ないという問題がある。
[Problems to be Solved by the Invention] Conventional skid prevention devices are configured as described above, so they can only be controlled after the tires actually begin to skid on the road surface, thereby preventing the vehicle from skidding. There is a problem in that the original and sufficient performance of prevention cannot be obtained.

然しながら予め路面の摩擦係数を検知し、これ
をデータとしてブレーキの掛かり具合を始めから
制御するように構成すれば効果的に横滑りを防止
できる横滑り防止装置を開発することが可能とな
る。
However, by detecting the friction coefficient of the road surface in advance and using this as data to control the degree of application of the brakes from the beginning, it becomes possible to develop a skid prevention device that can effectively prevent skids.

この発明はかかる課題を解決するためになされ
たもので、自動車の走行中に路面の摩擦係数を随
時検知してデータとして横滑り防止装置へ提供す
ることができる路面摩擦係数検知装置を得ること
を目的としている。
This invention was made in order to solve this problem, and the object is to obtain a road surface friction coefficient detection device that can detect the friction coefficient of the road surface at any time while the vehicle is running and provide it as data to the stability control device. It is said that

[課題を解決するための手段] この発明にかかる路面摩擦係数検知装置は、超
音波周波数を有するパルス状の電気信号を発生す
る送信機と、この電気信号を超音波に変換して路
面上へ向けて送出し、路面上で反射した反射波を
受信して電気信号に変換する送受波器と、受信し
た反射波のパルス幅を測定するパルス幅測定器と
を備え、自動車に搭載することとした。
[Means for Solving the Problems] A road surface friction coefficient detection device according to the present invention includes a transmitter that generates a pulsed electric signal having an ultrasonic frequency, and a transmitter that converts the electric signal into an ultrasonic wave and sends it onto the road surface. The device is equipped with a transducer that transmits the reflected wave toward the road surface, receives the reflected wave reflected on the road surface, and converts it into an electrical signal, and a pulse width measuring device that measures the pulse width of the received reflected wave. did.

[作用] 路面の摩擦係数は路面の硬さと関連し、路面の
硬さは超音波の反射係数と関連するので、反射波
のパルス幅を測定することで路面摩擦係数を検知
することが可能となる。
[Effect] The coefficient of friction of the road surface is related to the hardness of the road surface, and the hardness of the road surface is related to the reflection coefficient of ultrasonic waves, so it is possible to detect the coefficient of friction of the road surface by measuring the pulse width of the reflected waves. Become.

[実施例] 以下、この発明の実施例を図面について説明す
る。第1図はこの発明の一実施例である路面摩擦
係数検知装置の構成を示すブロツク図で、図にお
いて1は送信機、2は送受切替器、3は送受波
器、4は受信増幅器、5はパルス幅測定器であ
る。
[Example] Hereinafter, an example of the present invention will be described with reference to the drawings. FIG. 1 is a block diagram showing the configuration of a road surface friction coefficient detection device which is an embodiment of the present invention. In the figure, 1 is a transmitter, 2 is a transmitter/receiver switch, 3 is a transducer, 4 is a receiving amplifier, is a pulse width measuring instrument.

次に動作について説明する。送信機1で超音波
周波数を有する短いパルス状の電気信号を発生す
る。この電気信号は送受切替器2を経由して送受
波器3へ送られ、ここから超音波パルスとして空
中へ発射される。発射された超音波パルスは空中
を伝搬して路面へ到達し、路面上で反射して送受
波器3により反射波として受信される。
Next, the operation will be explained. A transmitter 1 generates a short pulse-like electrical signal having an ultrasonic frequency. This electrical signal is sent via the transmitter/receiver switch 2 to the transducer 3, from which it is emitted into the air as an ultrasonic pulse. The emitted ultrasonic pulse propagates through the air, reaches the road surface, is reflected on the road surface, and is received by the transducer 3 as a reflected wave.

第2図は送受波器3から発射される超音波パル
スの指向性の一例を示す図で、図において(D)は超
音波の指向性、各点(P0),(P1),(P2)は超音
波が到達する路面上の各位置、(R)は道路を示
す。第2図に示すように送受波器3から発射され
る超音波パルスは、サーチライトやフアンビーム
などの形状で、幅広い指向性(D)を持つが、送受波
器3の特性から、その垂直線上で対面する点
(P0)へは最大のエネルギーを持つた超音波パル
スが発射され、この垂直線上から角度θ1,θ2を有
する点(P1),(P2)方向へずれるに従つて、発
射される超音波のエネルギーは少ない。
Fig. 2 is a diagram showing an example of the directivity of the ultrasonic pulse emitted from the transducer 3. In the figure, (D) shows the directivity of the ultrasonic wave, and each point (P0), (P1), (P2) are each position on the road surface that the ultrasonic waves reach, and (R) indicates the road. As shown in Figure 2, the ultrasonic pulse emitted from the transducer 3 has a shape such as a searchlight or a fan beam, and has a wide directivity (D), but due to the characteristics of the transducer 3, its vertical Ultrasonic pulses with the maximum energy are emitted to the point (P0) facing each other on the line, and as they deviate from this vertical line toward points (P1) and (P2) having angles θ1 and θ2, they are emitted. The energy of ultrasonic waves is low.

また到達する超音波はその到達距離が長くなる
に従つて弱くなる。即ち距離0→1→2と
なるに従つて到達するエネルギーは弱くなる。
Furthermore, the arriving ultrasonic waves become weaker as the distance they reach becomes longer. In other words, as the distance increases from 0 to 1 to 2, the energy that arrives becomes weaker.

次に、このようにして道路(R)に到達した超
音波は、路面上の各点で反射され反射波が送受波
器3により受信されるが、この場合も送受波器3
への入射角が小さくなる各点に従つて、即ち
(P0)→(P1)→(P2)の順に弱くなる。
Next, the ultrasonic waves that have reached the road (R) in this way are reflected at various points on the road surface, and the reflected waves are received by the transducer 3. In this case as well, the transducer 3
The angle of incidence becomes smaller at each point, that is, in the order of (P0) → (P1) → (P2).

また路面上で反射される反射波の強度は、路面
の状況に依存する。即ち、路面が硬い場合には反
射強度も強く、路面が軟らかい場合には反射強度
も弱くなる。
Furthermore, the intensity of the reflected wave reflected on the road surface depends on the condition of the road surface. That is, when the road surface is hard, the reflection intensity is strong, and when the road surface is soft, the reflection intensity is weak.

このような条件下において送受波器3から受信
され、電気信号に変換され、受信増幅器4で増幅
された反射波は第3図に示すようになる。ここで
(R1)は軟らかい路面からの反射波の強度、
(R2)は硬い路面からの反射波の強度、(R0)は
予め定めたしきい値を示す。
Under such conditions, the reflected wave received from the transducer 3, converted into an electrical signal, and amplified by the reception amplifier 4 becomes as shown in FIG. Here, (R1) is the intensity of the reflected wave from the soft road surface,
(R2) indicates the intensity of reflected waves from a hard road surface, and (R0) indicates a predetermined threshold value.

第2図に示すように、送受波器3が垂直線上に
対面する点(P0)の位置から、出射角度θ1,θ2
となる点(P1),(P2)の方向にずれた場合、第
3図に示すように軟らかい路面(R1)からの反
射波の強度は点(P1)即ちθ1でしきい値以下に
なるが、硬い路面(R2)からの反射波の強度は
点(P2)即ちθ2までは、しきい値以上の値を示
す。
As shown in Figure 2, from the position of the point (P0) where the transducer 3 faces on the vertical line, the emission angles θ1, θ2
When shifted in the direction of points (P1) and (P2) where , the intensity of the reflected wave from the hard road surface (R2) shows a value above the threshold value up to point (P2), that is, θ2.

次に各点(P0),(P1),(P2)からの反射波の
到達時間について説明する。送受波器3から発射
された超音波が路面の各点(P0),(P1),(P2)
に当たつて反射して、反射波が再び送受波器3で
受信される、それぞれの時間tp0,tp1,tp2は、
空中における超音波の伝搬速度をvとすれば、そ
れぞれ2×0/v,2×1/v,2×2/
vとなる。また路面が硬い場合には、路面上の比
較的遠い地点(P2)から反射される反射波でも
比較的強く受信することができる。
Next, the arrival time of reflected waves from each point (P0), (P1), and (P2) will be explained. The ultrasonic waves emitted from the transducer 3 are transmitted to each point (P0), (P1), (P2) on the road surface.
The respective times tp0, tp1, tp2 at which the reflected waves are received by the transducer 3 are as follows:
If the propagation speed of ultrasonic waves in the air is v, then 2×0/v, 2×1/v, 2×2/
It becomes v. Furthermore, when the road surface is hard, even reflected waves reflected from a relatively far point (P2) on the road surface can be received relatively strongly.

従つて第4図に示すように硬い路面(R2)か
らのパルス幅(W2)は軟らかい路面(R1)から
のパルス幅(W1)に比べて{2×2/v}−
{2×1/v}だけの広がりを持つことになる。
Therefore, as shown in Fig. 4, the pulse width (W2) from the hard road surface (R2) is {2×2/v}− compared to the pulse width (W1) from the soft road surface (R1).
It has a spread of {2×1/v}.

従つて第1図に示すパルス幅測定器5で予め定
めた、しきい値(R0)を超えた反射波のパルス
幅(W)を測定することで、路面の摩擦係数にか
かる情報を予め横滑り防止装置へ情報として提供
することができる。
Therefore, by measuring the pulse width (W) of the reflected wave exceeding a predetermined threshold value (R0) using the pulse width measuring device 5 shown in FIG. It can be provided as information to the prevention device.

なお自動車の走行中における車体の振動が原因
による、送受波器3と道路(R)迄の距離の変動
による影響を避けるため、STC(感動時間制御)
を設けることにより、より精密を測定を行うこと
ができる。
In addition, in order to avoid the influence of changes in the distance between the transducer 3 and the road (R) caused by vibrations of the car body while the car is running, the STC (impression time control)
By providing this, more precise measurements can be made.

また送受波器3を路面に対し所定の角度を持つ
て取り付けることにより、路面状況に応じて適当
に検出感度を調整することが可能となる。
Furthermore, by attaching the transducer 3 at a predetermined angle to the road surface, it becomes possible to appropriately adjust the detection sensitivity depending on the road surface condition.

[発明の効果] この発明は以上説明したとおり、超音波を発射
して路面上から反射する反射波のパルス幅を測定
するという単純な方法で安価に路面摩擦係数を検
知することができ、自動車に搭載して走行中に随
時路面摩擦係数をデータとして横滑り防止装置へ
提供することができるので、横滑り防止装置で予
め路面の摩擦係数を検知してブレーキの掛かり具
合を堪案した上で制御することが可能になるとい
う効果がある。
[Effects of the Invention] As explained above, this invention enables the road surface friction coefficient to be detected at low cost by a simple method of emitting ultrasonic waves and measuring the pulse width of the reflected waves reflected from the road surface, and is useful for automobiles. The system can be installed on a vehicle and provide the road surface friction coefficient as data to the electronic stability control system at any time while driving, so the electronic stability control system can detect the friction coefficient of the road surface in advance and control the brakes after carefully considering the degree of application. This has the effect of making it possible.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図はこの発明の一実施例を示すブロツク
図、第2図は発射される超音波の指向性の一例を
示す図、第3図は反射波の強度を示す図、第4図
は路面状況の相違による反射波の相違を示す図。 1は送信機、2は送受切替器、3は送受波器、
4は受信増幅器、5はパルス幅測定器、R1は軟
らかい路面による反射波、R2は硬い路面による
反射波。なお、各図中同一符号は同一又は相当部
分を示すものとする。
Figure 1 is a block diagram showing an embodiment of the present invention, Figure 2 is a diagram showing an example of the directivity of emitted ultrasonic waves, Figure 3 is a diagram showing the intensity of reflected waves, and Figure 4 is a diagram showing the road surface. A diagram showing differences in reflected waves due to differences in situations. 1 is a transmitter, 2 is a transmitter/receiver switch, 3 is a transducer,
4 is a receiving amplifier, 5 is a pulse width measuring device, R1 is a reflected wave from a soft road surface, and R2 is a reflected wave from a hard road surface. Note that the same reference numerals in each figure indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】[Claims] 1 車輌に搭載され、超音波周波数を有するパル
ス状の電気信号を発生する送信機と、この電気信
号を超音波に変換し路面上へ向けて送出し路面上
で反射した反射波を受信して電気信号に変換する
送受波器と、この送受波器で受信した反射波のパ
ルス幅を測定するパルス幅測定器とを備えたこと
を特徴とする路面摩擦係数検知装置。
1. A transmitter mounted on a vehicle that generates a pulsed electric signal with an ultrasonic frequency, converts this electric signal into an ultrasonic wave, sends it out onto the road surface, and receives the reflected waves reflected on the road surface. A road surface friction coefficient detection device comprising: a transducer that converts into an electrical signal; and a pulse width measuring device that measures the pulse width of a reflected wave received by the transducer.
JP1056090A 1989-03-10 1989-03-10 Detector for frictional coefficient of road surface Granted JPH02236451A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1056090A JPH02236451A (en) 1989-03-10 1989-03-10 Detector for frictional coefficient of road surface

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1056090A JPH02236451A (en) 1989-03-10 1989-03-10 Detector for frictional coefficient of road surface

Publications (2)

Publication Number Publication Date
JPH02236451A JPH02236451A (en) 1990-09-19
JPH0549943B2 true JPH0549943B2 (en) 1993-07-27

Family

ID=13017399

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1056090A Granted JPH02236451A (en) 1989-03-10 1989-03-10 Detector for frictional coefficient of road surface

Country Status (1)

Country Link
JP (1) JPH02236451A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2837981B2 (en) * 1991-09-18 1998-12-16 日本無線株式会社 Automotive sensors
JP3440488B2 (en) * 1993-03-30 2003-08-25 マツダ株式会社 Road surface condition detection device in vehicle operation support system

Also Published As

Publication number Publication date
JPH02236451A (en) 1990-09-19

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