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Vibration Analysis and Modeling of Automobile Suspension Systems

Use these questions to demonstrate your individual ability to fulfill learning outcome criteria.

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Added on  2023-06-03

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This article discusses the modeling and analysis of single, double, and triple degree of freedom automobile suspension systems. It covers the equations of motion, natural frequencies, and damping ratios, as well as MATLAB implementation and Simulink models for system analysis. The article also includes information on vibration test rig control and roller mechanism applications.

Vibration Analysis and Modeling of Automobile Suspension Systems

Use these questions to demonstrate your individual ability to fulfill learning outcome criteria.

   Added on 2023-06-03

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DEMONSTRATION QUESTIONS
By (Name)
INSTITUTIONAL AFFILIATION
COURSE NAME & ID
PROFESSOR (INSTRUCTOR)
LOCATION (STATE, COUNTRY)
DATE OF SUBMISSION
1
Vibration Analysis and Modeling of Automobile Suspension Systems_1
SECTION A
QUESTION I: 1 DOF MODELLING
In the single DOF modeling, the acceleration of the automobile is a second derivative. The mass,
stiffness and damping of the SDOF system are represented using m, k, c which undergo the
relative displacement, velocity, and acceleration. The SDOF system and free body diagram is as
illustrated below,
The equation of motion,
m ̈x ( t )+ c ̇x ( t ) + kx ( t )=0
When it is normalized as a second order characteristic equation, it is expressed as,
̈x (t ) +2 ξ ω0 ̇x ( t )+ ω0
2 x ( t )=0
The damping ratio and the natural frequency of the SDOF system are given as,
ω0= k
m
ξ= c
2 mω0
For free vibration, the system is considered to have no external forces. Its response is given as,
x (t )= Asin ωn t+ B cos ωn t
For the damped case,
x (t )= ( A +Bt ) e( bt
2 m )
b=bcr=2 km=2 m ωn
2
Vibration Analysis and Modeling of Automobile Suspension Systems_2
For the under-damped case,
b< bcr
x ( t ) =e( bt
2 m ) ( A sin ωd t + B cos ωd t )
The damping natural frequency of the SDOF system is given as,
ωd=ω0 1ξ2
For the forced vibration, there is an external force towards the SDOF system, and the general
solution to the characteristic equation is obtained as,
̈x ( t ) + k
m x ( t ) + c
m ̇x ( t ) =Fsin ωt
x (t )= F sin ωt +θ
k
(1
( ω2
ωn
2 ) )+ ( 2 ξω
ωn )2
¿ F
k
( sin ωt +θ
( 1 ( ω2
ωn
2 ) ) +
( 2 ξω
ωn )
2
)
Road surface automobile suspension response,
Using the modeled uneven road surface, a vehicle can be driven at speeds ranging from 0 to
65kph to avoid too much rumbling and discomfort of the passengers,
3
Vibration Analysis and Modeling of Automobile Suspension Systems_3
MATLAB implementation of the SDOF System
(i) Obtaining the system Laplace transform and developing a transfer function
(ii) Generating a Simulink model of the system
(iii) Performing several analysis on bode diagrams of the system response, magnification
and transmissibility factor, and derivation of some parameters.
The code snippet
%% SDOF System analysis
m=45e3; % 45000 kg
k=35e3; % stiffness of the spring
c=18500; % damping coefficient, of the damper
% Using matrix form of the SDOF system to generate the
transfer function
A=tf([m c k],[1]) % The transfer function, A
B=tf([c k],[1]) % The transfer function, B
sys=B/A % The transfer function, The system
%% Using the step function to determine the system response
figure(2)
step(sys)
grid on
%% To determine the system magnitude and phase plot using bode
diagram
figure(3)
bode(sys)
grid on
%% The natural frequency and the damping factor of the
calculations in the system
[Wn, zeta]=damp(sys)
4
Vibration Analysis and Modeling of Automobile Suspension Systems_4

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