Passenger cars — Braking in a turn — Open-loop test procedure

Specifies an open-loop test procedure to determine the effect of braking on course holding and directional behaviour if a vehicle whose steady-state circular motion is altered by a braking action only.

Voitures particulières — Freinage en virage — Méthode d'essai en boucle ouverte

General Information

Status
Withdrawn
Publication Date
25-Dec-1996
Withdrawal Date
25-Dec-1996
Technical Committee
Drafting Committee
Current Stage
9599 - Withdrawal of International Standard
Completion Date
29-Mar-2006
Ref Project

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ISO 7975:1996 - Passenger cars -- Braking in a turn -- Open-loop test procedure
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INTERNATIONAL IS0
STANDARD 7975
Second edition
1996-I 2-l 5
Passenger cars - Braking in a turn -
Open-loop test procedure
Voitures particuli&es - Freinage en virage - M&hode d’essai en boucle
ouverte
Reference number
IS0 7975: 1996(E)

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IS0 7975: 1996(E)
Foreword
IS0 (the International Organization for Standardization) is a worldwide
federation of national standards bodies (IS0 member bodies). The work of
preparing International Standards is normally carried out through IS0
technical committees. Each member body interested in a subject for which
a technical committee has been established has the right to be rep-
resented on that committee. International organizations, governmental and
non-governmental, in liaison with ISO, also take part in the work. IS0
collaborates closely with the International Electrotechnical Commission
(IEC) on all matters of electrotechnical standardization.
Draft International Standards adopted by the technical committees are
circulated to the member bodies for voting. Publication as an International
Standard requires approval by at least 75 % of the member bodies casting
a vote.
International Standard IS0 7975 was prepared by Technical Committee
ISO/TC 22, Road vehicles, Subcommittee SC 9, Vehicle dynamics an
road-holding ability.
This second edition cancels and replaces the first edition (IS0 7975:1985 1)
I
which has been technically revised.
Annexes A and B form an integral part of this International Standard.
0 IS0 1996
All rights reserved. Unless otherwise specified, no part of this publication may be reproduced
or utilized in any form or by any means, electronic or mechanical, including photocopying and
microfilm, without permission in writing from the publisher.
International Organization for Standardization
Case postale 56 l CH-1211 Geneve 20 l Switzerland
Printed in Switzerland
ii

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IS0 7975: 1996(E)
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Introduction
The dynamic behaviour of a road vehicle is a most important part of the
active vehicle safety. Any given vehicle, together with its driver and the
prevailing environment, constitutes a closed-loop system which is unique.
The task of evaluating the dynamic behaviour is therefore very difficult,
since the significant interaction of these driver-vehicle-road elements are
each complex in themselves. A description of the behaviour of the road
vehicle must inevitably involve information obtained from a number of
tests of different types.
Since the braking in a turn test procedure quantifies only one small part of
the complete handling characteristics, the results of this test can only be
considered significant for a correspondingly small part of the overall
dynamic behaviour.
Moreover, insufficient knowledge is available concerning the relationship
between overall vehicle dynamic properties and accident avoidance. A
large amount of work is necessary to acquire sufficient and reliable data on
the correlation between accident avoidance and vehicle dynamic properties
in general and the results of this test in particular. Therefore, it is not
possible to use this procedure for regulation purposes.
. . .
III

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INTERNATIONAL STANDARD 0 IS0 IS0 7975:1996(E)
Passenger cars - Braking in a turn - Open-loop test
procedure
1 Scope
This International Standard specifies an open-loop test procedure to determine the effect of braking on course
holding and directional behaviour of a vehicle whose steady-state circular motion is altered by a braking action only.
It applies to passenger cars as defined in IS0 3833.
2 Normative references
The following standards contain provisions which, through reference in this text, constitute provisions of this
International Standard. At the time of publication, the editions indicated were valid. All standards are subject to
revision, and parties to agreements based on this International Standard are encouraged to investigate the
possibility of applying the most recent editions of the standards indicated below. Members of IEC and IS0
maintain registers of currently valid International Standards.
IS0 1176: 1990, Road vehicles - Masses - Vocabulary and codes.
IS0 3833:1977, Road vehicles - Types - Terms and definitions.
IS0 4138: 1996, Passenger cars - Steady-state circular driving behavi’our - Open-loop test procedure.
IS0 8855:1991, Road vehicles - Vehicle dynamics and road-holding ability - Vocabulary.
3 Principle
The purpose of this test procedure is to determine the effect of braking on course holding and directional behaviour
of a vehicle, whose steady-state circular motion is disturbed by a braking action only.
The initial conditions are defined by constant longitudinal velocity and by a circle with a given radius. The steering-
wheel angle required for the steady-state circular run shall be constantly maintained during the entire test. During
the test the driver input and the vehicle response are measured and recorded. From the recorded signals,
characteristic values are calculated.
The variables of motion used to describe the effect of braking on course holding and directional behaviour of the
vehicle relate to the intermediate axis system XI Yf Z (see IS0 8855).
1

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IS0 7975: 1996(E) @ IS0
The location of the origin of the intermediate axis system, being the reference point, is independent from loading
condition. It is fixed in the longitudinal plane of symmetry at half wheelbase and at the same height above the
ground as the centre of gravity of the vehicle at complete vehicle kerb mass (see IS0 1176).
4 Variables
The following variables shall be measured:
- moment of brake application, to;
- steering-wheel angle, &Hi
- lateral acceleration, ay;
- longitudinal acceleration, ax;
- longitudinal velocity, vx;
- yaw velocity, *.
It is recommended to measure the following variables as well:
- pressure at master cylinder output or in the brake circuit which activates at least one of the front wheel
brakes, PB;
- roll angle, (p;
- pitch angle, 8;
- sideslip angle, p;
or lateral velocity, vy;
- stopping distance, sB;
- wheel rotation speed, o1 - ~0~.
The variables are defined in IS0 8855 except the stopping distance, the brake pressure and the moment of brake
application to, which is the instant at which the brake pedal is operated. Alternatively the actuation of the brake
light switch may be used to specify the moment of brake application to.
5 Measuring equipment
5.1 Description
The variables selected from those listed in clause 4 shall be measured by means of appropriate transducers and
their time histories shall be recorded by a multi-channel recorder. This does not obligatorily apply to stopping
distance, which can be measured directly after the test has been completed. The typical operating ranges and
recommended maximum errors of the transducer and recording system are shown in table 1. The values in table 1
are tentative and provisional until more experience is available.
5.2 Transducer installation
The transducers shall be installed according to the manufacturer’s instructions where such instructions exist, so
that the variables corresponding to the terms and definitions of IS0 8855 can be determined.
If the transducer does not measure the values directly, appropriate transformations into the reference system shall
be carried out.
2

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@ IS0 IS0 7975: 1996(E)
Table 1 - Measured variables, their typical operating ranges and
recommended maximum errors
Variable Typical operating range
Longitudinal velocity 0 m/s to 50 m/s k 0,5 m/s
- 5O”/s to + 5O”/s
Yaw velocity +, 0,5”/s
30 MPal)
Pressure of braking system + 0,3 MPal)
- 15O to + 15”
Roll angle f0,15”
- 15O to + 15O &0,15O
Pitch angle
- 20” to + 20” + 0,5O
Sideslip angle
Lateral velocity -10m/sto+10m/s +O,l m/s
Stopping distance 300 m + 0,5 m
Wheel rotation speed 0 s-l to 200 s-l k 2 s-l
1) 1 Mpa=10bar=106N/m2
Transducers for measuring some of the listed variables are not widely available and are not in
NOTE -
general use. Many such instruments are developed by users. If any system error exceeds the recommended
maximum values, this and the actual maximum error shall be stated in the test report (see annex A).
. Data processing
53
The frequency range relevant for this test is between 0 Hz and the maximum utilized frequency of fmax = 5 Hz.
According to the chosen data processing method, analog or digital, the stipulations given in 5.3.1 or 5.32 shall be
observed.
5.3.1 Analog data processing
The bandwidth of the entire combined transducer/recording system shall be no less than 8 Hz.
In order to execute the necessary filtering of signals, low-pass filters with order four or higher shall be employed.
The width of the passband frequency fo at -3 dB shall not be less than 8 Hz. Amplitude errors shall be less than
+ 0,5 % in the relevant frequency range of 0 Hz to 5 Hz. All analog signals shall be processed with filters having
sufficiently similar phase characteristics, in order to ensure that time delay differences due to filtering lie within the
required accuracy for time measurement.
NOTE - Phase shifts may occur during analog filtering of signals with different frequency contents. Therefore a data
processing method, as described in 5.3.2, is preferable.
53.2 Digital data processing
5.3.2.1 Preparation of analog signals
In order to avoid aliasing, the analog signals shall correspondingly be filtered before digitizing. In this case, low-pass
filters with order four or higher shall be employed. The width of the passband (frequencyfo at -3 dB) shall amount
to roughly

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IS0 7975:1996(E)
The amplitude error of the anti-aliasing filter should not exceed + 0,5 % in the utilized frequency range from zero to
All analog signals shall be processed with anti-aliasing filters having sufficiently similar phase characteristics in
f max-
order to ensure that time delay differences lie within the required accuracy for time measurement.
Additional filters shall be avoided in the data acquisition string.
Amplification of the signals shall be such that, in relation with the digitizing process, the additional error is less than
0,2 %.
5.3.2.2 Digitizing
The sampling rate fS shall be appropriate to the order of the filters being used and shall under no circumstances be
less than ;rfo.
NOTE - In common practice anti-aliasing filters of Butterworth type are used. For this type of filter the following
specifications are recommended:
four pole filter: fS 2 sfo
eight pole filter: fS 2 3,6fo
5.3.2.3 Digital filtering
For filtering of sampled data in data evaluation, phaseless (zero phase shift) digital filters shall be used incorporating
the following characteristics (see figure 1):
- passband range, 2 0 Hz to > 5 Hz;
~4OHzand~15Hz;
- start of stopband,
- filter gain in the passband, 1 L- 0,005 (100 % + 0,5 %);
- filter gain in the stopband, G 0,Ol (S 1 %).
Stopband
Frequency, Hz
Figure II - Required characteristics of phaseless digital filters
4

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6 Test conditions
Limits and specifications for the ambient and vehicle test conditions are established in 6.1 to 6.3, and shall be
maintained during the test. Any deviations shall be shown in the test report (see annex A), including the individual
diagrams of the presentation of results (see annex B).
road friction
NOTE - The ambient temperature m ay influence both the and the tyre characteristics. Therefore the tests
thout the ambie nt temperature varying too much.
should be carried out wi
6.1 Test track
All tests shall be carried out on a level, clean and uniform hard road surface, which must not exceed a gradient of
2,5 % at any place. For standard test conditions, a smooth dry road pavement of asphalt or concrete or a high
friction test surface is recommended.
6.2 Wind velocity
The wind velocity shal I not exceed 5 m/s and shall be recorded in the test report (annex A).
6.3 Test vehicle
6.3.1 Tyres
For standard tyre condition, new tyres shall be fitted on the test vehicle according to the manufacturer’s
specifications. They shall have a tread depth of at least 90 % of the original value and shall be manufactured not
more than one year before the test.
Tyres shall be inflated to the pressure as specified by the vehicle manufacturer for the test vehicle configuration at
the ambient temperature. The tolerance for setting the cold pressure is + 5 kPal) for pressures up to 250 kPa and
+ - 2 % for pressure above 250 kPa.
They shall be run in for at least 150 km without excessively harsh use, for example braking, acceleration, cornering,
hitting the kerb, etc. After the tyres have been run in, they should remain in the same position on the vehicle for
the test.
The test may also be performed with tyres in any state of wear as long as the end of the test they are in such a
condition that a minimum of I,6 mm of tread depth remains across the whole breadth of the tread (see note) and
around the whole circumference of tyre.
NOTES
which with the tyre correctly inflated contacts the road in normal
Tread breadth is the width of that part of the tread
str .aight-line drivin
9
2 Asin certain cases the tread depth has a significant infl uence on test results, it is recommended that it should be taken into
etween tyres.
account when making comparisons betwe en vehicles or b
6.3.2 Operating components
For standard test conditions, all operating components likely to influence the results of this test (for example
condition, setting and temperature of shock absorbers, springs and other suspension components and suspension
geometry) shall be as specified by the manufacturer. Any deviations from manufacturer’s specification shall be
noted in the test report (see the annex A).
The b rakes shall be bedded fully and correct accordin g to procedu res specified by the vehicle ma nufacturer or to
IY
sed shall be indicated in t he test report (see annex A)
other availa ble spec ifications. The procedure U
1) 1 kPa = 1 O-* bar = 1 O3 N/m*

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6.3.3 Engine and drivetrain
For standard test conditions, the adjustment and condition of the engine and the drivetrain (especially the
differentials, clutches, locks and free wheel shifts) shall correspond to the vehicle manufacturer’s specifications.
6.3.4 Loading conditions of the vehicle
The test mass shall be between complete vehicle kerb mass (code: ISO-M06) plus driver’s mass and maximum
authorized total mass (code: ISO-M08). The instrumentation plus driver should preferably not exceed 150 kg.
The maximum authorized total mass and the maximum authorized axle loads (code: ISO-M13) shall lot be
exceeded.
Care shall be taken to generate the minimum deviation in the location of the centre of gravity and in the va ues of
the moments of inertia as compared to the loading conditions of the vehicle in normal use. The resulting wheel
loads shall be determined and recorded in the test report (annex A).
7 Test procedure
7.1 Tyre warm-up
The tyres shall be warmed up in order to achieve a tyre temperature and pressure representative of normal driving
conditions. This should be done by driving at a speed of 100 km/h over a distance of at least 10 km. However, if
this is not practicable, it may be done by driving 500 m at a lateral acceleration of 3 m/s* on the radius to be used
for the tests. The tyre pressures after warm-up should be recorded.
7.2 Brake temperature
At the beginning of the test, the braking system shall be warmed up to its operating temperature by performing
some consecutive stops.
Prior to each test run the temperature of the brake discs and drums shall be measured to ensure an initial brake
temperature of less than 100 “C.
7.3 Initial driving condition
The initial driving condition is that of the steady-state circular test (see IS0 4138) with the initial conditions relating
to the combinations of radii and lateral acceleration given in table 2. During this procedure the vehicle shall be
steered in such a manner that the reference point of the vehicle moves on the desired circular path. As it is known
that the significance of the results and the discrimination between different vehicles increase with increasing test
speed, the standard radius of this path shall be 100 m. Smaller radii ranging from 30 m to 50 m with 40 m as the
recommended lower value may be used. Additional tests using a radius of 200 m are recommended.
For vehicles with manual transmission the test shall be performed in the highest gear compatible with the
conditions of the test given in table 2. For vehicles with automatic transmission the position of the transmission
lever and the selected driving program shall be recorded in the test report (see annex A).
The position of the steering-wheel and the accelerator pedal shall be kept as constant as possible during the initial
driving condition. The initial condition is considered to be sufficiently constant, if one of the following conditions is
fulfilled:
a) for the time interval from I,3 s to 0,3 s before brake application the standard deviation of the lateral
acceleration shall not exceed 5 % of the mean value and the standard deviation of the longitudinal velocity shall
not exceed 3 % of the mean value;
b) the difference between the mean values during the time intervals I,3 s to 0,8 s and 0,8 s to 0,3 s before brake
application shall not exceed the last mentioned mean value for the lateral acceleration by 5 % and for the
longidudinal velocity by 3 %.
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The radius in the initial driving condition may not deviate by more than + 0,5 m of the desired value during the time
interval of I,3 s to 0,3 s before brake application. The initial radius R, is calculated as follows:
2
vxo vxo
=I
Ro =-+- or R.
aY,O
YO
Table 2 - Initial test conditions
Corresponding
Condition Radius Lateral acceleration
longitudinal velocity
m m/s* tol., % km/h tol., %
Standard 100 5 &IO 81 +5
Option 200 5 k10 114 k5
I 1 30to50 1 5 1 &IO 1 44to57 1 +5
7.4 Performance of the braking procedure
When the initial steady-state driving condition has been reached, the steering-wheel is fixed by a mechanical
device or, alternatively, is firmly held by the driver. The accelerator pedal shall be released and brakes applied as
quickly as possible. On vehicles with manual transmission, the clutch may be disengaged immediately or at the
end of the test run; the option chosen shall be indicated in the test report (see annex A). On vehicles with
automatic transmission the shift lever remains in the initial position.
The actuation of the brake pedal or the brake light switch is considered as the moment of brake application to.
During braking the pressure in the braking system or the brake pedal force or the brake pedal travel shall be kept
as constant as possible (an adjustable stop under the brake pedal may serve) and the steering-wheel shall be fixed
until the test run is finished.
The test runs for each combination of radius and lateral acceleration defined in table 2 shall be made at increasing
levels of longitudinal acceleration until, on vehicles with conventional braking system, lock up of at least one of the
front wheels occurs (if possible). The test may be continued beyond this point resulting in further wheels locking
until lock up of all wheels has occurred, but testing under these conditions may result in rapid and large changes of
tyre characteristics, which may cause wide variations in test results. On vehicles equipped with an antilock braking
system the test shall be continued until the peak value of mean longitudinal acceleration at time t, (see 8.3.4) is
detected.
The minimum braking action shall correspond to a mean longidutinal acceleration of 2 m/s2 and shall then increase
by increments of not more than 1 m/s? if the results vary rapidly with longitudinal acceleration smaller increments
should be selected.
Tests shall be carried out for both left- and right-hand turns.
The transducer signals shall be recorded from I,3 s before brake application until the vehicle comes to a standstill.
This recording period shall be extended by the setting time of all filters used during recording
depending on the type of filter used).
steady-state
During the recording period the steering-wheel angle shall not deviate more than + 3 % from the
ee times.
value. To increase accuracy it is recommended that the series of tests should be performed at least th
8 Data evaluation and presentation of results
8.1 General
General data shall be presented in the test report as shown in annex A. For every change in equipment of the
vehicle (e.g. load), the general data shall be documented again.

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IS0 7975:1996(E)
Due to the large amount of data, the use of a computer for data processing is recommended.
At the present level of knowledge, it is not yet known which variables best represent the subjective feeling of the
driver and which variables, i.e. what characteristic values best describe the dynamic reaction of vehicles. The
following specified variables therefore represent only examples for the evaluation of results.
8.2 Time histories
For every test run, time histories of the variables listed in clause 4 shall be presented. Apart from their evaluation
purposes, the time histories serve to monitor correct test performance and functioning of the transducers.
8.3 Braking action
8.3.1 Reference point in time t0
The reference point in time t0 for the following characteristic values is the moment of brake pedal actuation or the
actuation of the brake light switch.
8.32 Definition of times and requirements
Figure 2 shows the pattern of longitudinal acceleration during braking versus time.
Time interval
for evaluation
- I
Figure 2 - Definition of times
8

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For the correct performance of a test run, the rise time of the longitudinal acceleration shall not exceed 0,4 s. The
rise time is defined as the difference between the reference point in time to and the time tgo. Time tg0 is the time
when the longitudinal acceleration reaches 90 % of the value at 1 s after the time to. The longitudinal acceleration
at 1 s after the time to is evaluated by taking the mean value during the time interval 0,9 s and 1 ,I s and after to.
The time tf is defined as the time when the longitudinal acceleration reaches the value zero at the end of the
braking actuation.
8.3.3 Mean longitudinal acceleration - Ex
The mean longitudinal acceleration is the average value of longitudinal acceleration measured during each brake
application.
This average value may be obtained by either:
a) measuring the distance needed by the vehicle to stop from instant to, in which case the mean longitudinal
acceleration is given by:
2
‘/eff
=-
-qf
2x seff
where
is the actual stopping distance, in metres;
Seff
is the actual initial velocity, in metres per second;
Veff
b) taking the mean value during the time interval to to lf of the longitudinal acceleration (see figure 3).
Longitudinal acceleration -ax versus time
Figure 3 -

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IS0 7975: 1996(E) @ IS0
8.3.4 Mean longitudinal acceleration ---ax t until time t”
t n
The mean longitudinal acceleration at any time tn after brake application is defined as the mean value during the
time interval lo to tn of the longitudinal acceleration (see figure 3).
8.4 Characteristic values
The characteristic values shall be determined and presented as a function of the mean longitudinal acceleration or
the mean longitudinal acceleration at time tn (see 8.3.3 and 8.3.4). The characteristic values in the steady-state
condition are defined as mean values during the time interval I,3 to 0,3 s before brake application. The other
characteristic values are determined during an observation period beginning at to and ending with the standstill of
the vehicle. The instantaneous values at tn shall be calculated by taking the mean value during the time interval t,
from -0,l s to +O,l s. For standard evaluation the actual time is tn = to + 1 s, but tn may also assume additional
values.
For each set of initial conditions, calculate and plot the characteristic values listed below. The reference values of
yaw velocity and lateral acceleration used in some of the formulas are those values which would be obtained at
if the initial radius were maintained by the vehicle. They are
actual time t and actual longitudinal velocity vx,t,
defined as follows:
.
Vxt
Reference yaw velocity:
yRef,t =I
RO
2
Vxt
Reference lateral acceleration: ay Ref t =A
I I
RO
8.4.1 The ratio of the maximum value attained by the yaw velocity during braking to the initial steady-state value
of the yaw velocity (see figure B.l):
Y
max
.
-=f1 (-ax,
6
8.4.2 The ratio of the maximum value attained by the latera I acceleration during braking to the initial steady-state
value of the lateral acceleration (see figure B.2):
aY max
L=f2 (-ax)
ar,o
8.4.3 The ratio of the maximum value attained by the sideslip angle during braking to the initial steady-state value
of the sideslip angle (see figure B.3):
P max
-----=f3 (-a,,
PO
8.4.4 The maximum value of the difference between the yaw velocity during braking and the affiliated reference
yaw velocity (see figure B.4):
, I,,,= [% -Jglmax =fi(-~x)
ALj/max = [*t -*Ref t
8.4.5 The ratio of the mean values of the yaw velocity during braking to the reference yaw velocity (see
figure B.5):
iF i?
-=-~f5 (-ax)
(*i/2)
FRef
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8.4.6 The difference between the values of the yaw velocity at actual time tn and the reference yaw velocity at
actual time tn (see figure B.6):
zx q - qn Ref= 5
- -=fG(-qyt
A\y,
f n
n n n
,
RO
the lateral acceleration at actual time tn and the reference lateral
8.4.7 The difference between the values of
acceleration at actual time tn (see figure B.7):
2
‘Xfn
--=f7(-ax,t,)
AaY, tn = aY, tn - aY, tn,R& = aYt tn
RO
8.4.8 The difference between the values of the yaw velocity at actual time tn and the calculated yaw velocity at
actual time tn (see figure B.8):
p;, = etn - !%!2- = f* (-ax, t, )
‘X fn
where @ is the sideslip angle velocity uncorrected for the effects of the sideslip angle itself and the deceleration.
It gives information on the vehicle’s yaw stability.
8.4.9 The ratio of the value of the initial radius to the path radius of the vehicle’s reference point at actual time tn
(see figure B.9):
RO
-=
fg (-‘X, tn )
Rt
n
2
‘Xtn
=-
Rt
n
aYt
1 n
8.4.10 The ratio of the value of the yaw velocity at actual time tn to the initial steady-state value of the yaw
velocity (normalized yaw velocity at actual time) (see figure B.lO):
II;
n
.
-=fiO (-‘X,tn)
‘yo
8.4.11 The ratio of the value of the lateral acceleration at actual time tn to the initial steady-state value of the
lateral acceleration (normalized lateral acceleration at actual time) (see figure B.ll):
aYt
1 n
-=f&~x,t,)
aY, 0
8.4.12 The difference between the values of the sideslip angle at actual time tn and the initial steady-state value
of the sideslip angle (see figure B.12):
fit,- PO=fl2 ‘-‘X,tn’
11

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IS0 7975:1996(E)
8.4.13 The difference between the values of the yaw angle at actual time tn and the value of the reference yaw
angle at actual time tn (see figure B.13).
Approximation:
‘0 + *tn Ref
AYt =Yt ’
=h3(-ax,tn)
n n
2
I
Exact solution:
t=tn
*g -*R&t dt
alu, =
n 9
1
t=to
8.4.14 The path deviation at actual time tn defined as the radial distance of the reference point and its initial
circular path (see figure B.14):
hxtn = fi 4 (-‘X,tn)
The path deviation is calculated by the path of the reference point in the earth fixed axis system (see figure 4). The
coordinates of the reference point can be determined for example by transforming the vehicle fixed velocity
vectors ?x and Ty into the earth fixed axis system and subsequent integration.
Figure 4 - Definition of path deviation

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8.5 Criteria for vehicle behaviour
The behaviour of the vehicle in this test can be described under the headings steerability and yaw behaviour as a
function of the braking characteristics.
8.5.1 Steerability
Criteria which may be used amongst others to describe steerability are:
a) the value of mean longitudinal acceleration -ZX, at actual time t, at which the normalized lateral acceleration
’ n
at actual time (see 8.4.11) reaches the value zero;
NOTE - This criteria is not applicable to ABS systems.
the value of mean longitudinal acceleration -ZX, at actual time t, at which the normalized lateral acceleration
b)
’ n
at actual time reaches the normalized reference value (see figure 5). The normalized reference value can be
approximately defined according to the equation
2
-ax t x ct, -to)
5,O -
’ n
ayltn Ref i [ II
A=
NOTE - The criteria listed above assume a vehicle equipped with a convention
...

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