JPH02236451A - Detector for frictional coefficient of road surface - Google Patents

Detector for frictional coefficient of road surface

Info

Publication number
JPH02236451A
JPH02236451A JP1056090A JP5609089A JPH02236451A JP H02236451 A JPH02236451 A JP H02236451A JP 1056090 A JP1056090 A JP 1056090A JP 5609089 A JP5609089 A JP 5609089A JP H02236451 A JPH02236451 A JP H02236451A
Authority
JP
Japan
Prior art keywords
road surface
ultrasonic
reflected
pulse width
transmitter
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.)
Granted
Application number
JP1056090A
Other languages
Japanese (ja)
Other versions
JPH0549943B2 (en
Inventor
Chogo Sekine
兆五 関根
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

Abstract

PURPOSE:To perform the control in consideration of the braking condition and to inexpensively detect the frictional coefficient of the road surface by emitting an ultrasonic wave and measuring the pulse width of the reflected wave from the road surface. CONSTITUTION:A short pulse electric signal having an ultrasonic frequency is generated by a transmitter 1. This electric signal is sent to a transmitter- receiver 3 through a transmission/reception switch 2 and is radiated to air from the transmitter-receiver 3 as an ultrasonic pulse. This ultrasonic pulse is propagated in air and reaches the road surface and is reflected on the road surface and is received as the reflected wave by the transmitter-receiver 3. Since the frictional coefficient of the road surface is related to the hardness of the road surface and this hardness is related to the reflection coefficient of the ultrasonic wave, the pulse width of the reflected wave is measured by a pulse width measuring part 5 to detect the frictional coefficient of the road surface.

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
掌擦係数検知装置に関するものである。
[Detailed Description of the Invention] [Industrial Application Field] This invention relates to a road surface palm 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 the road surface while driving. It is related to.

「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
により車輪がロッ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A
 L B (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'' A method of electronically controlling the degree of braking in order to prevent the wheels from locking due to road surface conditions and causing a skid when sudden braking is applied while the vehicle is in motion.
A skid prevention device called LB (anti-lock 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っ
て自動車の走行スピ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 the system works, the tires will slip on the road surface, making it difficult to control the vehicle's speed. Furthermore, if the tires start to skid in this way, the braking force of each tire is different, causing the car 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.

然しなか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 brake application 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コ 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] The 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 this electric signal into an ultrasonic wave and transmits it onto the road surface. Send it towards
It is equipped with a transducer that receives reflected waves reflected from the road surface and converts them into electrical signals, and a pulse width measuring device that measures the pulse width of the received reflected waves, and is installed in a car.

[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.

[実施例コ 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
構成を示すブロック図で、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. 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。
[Embodiments] Hereinafter, embodiments of the present invention will be described with reference to the drawings. 1st
The figure 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 receiver amplifier, and (5) is a pulse width measuring device. Next, the operation will be explained. A transmitter (1) generates a short pulsed electrical signal having an ultrasonic frequency. This electrical signal is sent to the transducer (3) via the transceiver switch (2), and is emitted into the air as an ultrasonic pulse from there. 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(PO).(Pi),(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、サーチライトやファンビームなどの形状で、幅広
い指向性(D)を持つが、送受波器ク3)の特性から、
その垂直線上で対面する点(PO)へは最大のエネルギ
ーを持っ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(PL),(P2)方向へず
れるに従って、発射される超音波のエネルギーは少ない
. また到達する超音波はその到達距離が長くなるに従って
弱くなる。即ち距離OPO→OPI→OP2となるに従
って到達するエネルギーは弱くなる. 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って、即ち(PO)→(P1)→(
P2)の順に弱くなる。
FIG. 2 is a diagram showing an example of the directivity of ultrasonic pulses emitted from the transducer (3). In the figure, (D) shows the directivity of the ultrasonic waves at each point (PO). (Pi) and (P2) indicate each position on the road surface that the ultrasonic waves reach, and (R) indicates the road. As shown in Figure 2, the ultrasonic pulses emitted from the transducer (3) have the shape of a searchlight or fan beam, and have a wide range of directivity (D), but the characteristics of the transducer (3) from,
Ultrasonic pulses with the maximum energy are emitted to the point (PO) facing each other on the vertical line, and the ultrasonic pulses are emitted as they deviate from this vertical line toward points (PL) and (P2) having angles θ1 and θ2. The energy of ultrasonic waves is low. Furthermore, the ultrasonic waves that arrive become weaker as the distance they reach becomes longer. In other words, as the distance increases from OPO to OPI to OP2, the energy that arrives becomes weaker. Next, the ultrasonic waves that reached the road (R) in this way are
The waves reflected at each point on the road surface are received by the transducer (3), but in this case as well, the angle of incidence on the transducer (3) decreases according to each point, that is, (PO) → (P1 )→(
P2) becomes weaker in this order.

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. In other words, when the road surface is hard, the reflection intensity is strong,
When the road surface is soft, the reflection intensity also becomes weaker.

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、(RO)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 receiving amplifier (4) becomes as shown in FIG. Here, (R1) represents the intensity of the reflected wave from the soft road surface, (R2) represents the intensity of the reflected wave from the hard road surface, and (RO) represents 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(PO)の位置から、出射角度θ1θ2となる点
(Pi),(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(R
2)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 Fig. 2, when the transducer (3) deviates from the position of the point (PO) facing each other on the vertical line in the direction of the points (Pi) and (P2) where the emission angle is θ1θ2, the third As shown in the figure, the intensity of the reflected wave from the soft road surface (R1) is at the point (
P1), that is, θ1 is below the threshold value, but on a hard road surface (R
The intensity of the reflected wave from 2) up to point (P2), that is, θ2, is:
Indicates a value above the threshold.

次に各点(PO),(PL),(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(po),(PI),(P2)
に当たって反射して、反射波が再び送受波器(3)で受
信される、それぞれの時間tpo,tpl,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
2xopo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, we will explain the arrival time of the reflected waves from each point (PO), (PL), (P2>.The ultrasonic wave emitted from the transducer (3) reaches each point (PO), (PI) on the road surface. , (P2)
The respective times tpo, tpl, 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 if the road surface is hard, even a reflected wave reflected from a relatively far point (P2) on the road surface can be received relatively strongly.

従って第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(Rl)からのパルス幅(
W1)に比べて{2×oP2/■}一{2×○P 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 different from the pulse width (W2) from the soft road surface (Rl).
W1) compared to {2×oP2/■}-{2×○P 1
/v).

従って第1図に示すパルス幅測定器(5)で予め定めた
、しきい値(RO)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 that exceeds a predetermined threshold value (RO) using the pulse width measuring device (5) shown in Figure 1, information regarding the friction coefficient of the road surface can be obtained in advance. It can be provided as information to the stability control 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 (ffi度時間制御)を設ける
ことにより、より精密な測定を行うことができる。
Please note that this is caused by the vibration of the car body while the car is running.
In order to avoid the influence of changes in the distance between the transducer (3) and the road (R), more precise measurements can be made by providing STC (ffi degree time control).

また送受波器(3)を路面に対し所定の角度を持って取
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
がり具合を勘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 vehicle after taking into account the degree of brake application. This has the effect of making it possible.

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

第1図はこの発明の一実施例を示すブロック図、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。 lit図 m2図
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. lit diagram m2 diagram

Claims (1)

【特許請求の範囲】[Claims] 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。
A transmitter mounted on a vehicle generates a pulsed electrical signal with an ultrasonic frequency, converts this electrical signal into an ultrasonic wave, sends it out onto the road surface, receives the reflected waves reflected on the road surface, and generates electricity. A road surface friction coefficient detection device comprising: a transducer that converts into a 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 true JPH02236451A (en) 1990-09-19
JPH0549943B2 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)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0579839A (en) * 1991-09-18 1993-03-30 Japan Radio Co Ltd On-vehicle sensor
JPH06281539A (en) * 1993-03-30 1994-10-07 Mazda Motor Corp Road surface condition detection device of steering support system of motor vehicle

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0579839A (en) * 1991-09-18 1993-03-30 Japan Radio Co Ltd On-vehicle sensor
JPH06281539A (en) * 1993-03-30 1994-10-07 Mazda Motor Corp Road surface condition detection device of steering support system of motor vehicle

Also Published As

Publication number Publication date
JPH0549943B2 (en) 1993-07-27

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