Quarter car suspension model The figure below a model of the suspension of a car. r(t)is the position of the mass of the car from its equilibrium position while z is the profile of the road. Note that z is a function of the distance y along the road, but you need (t) which you can obtain from z(y) using the chain rule. The car is traveling to the right on the road at a speed v. Assume the mass of the car is 250 kg, the spring constant is 16 kN/m, and damping constant is 1000 Ns/m. (a) Derive the differential equation for the position of the car r(t). (b) If z(t) Zoejwot, determine the amplitude and the phase of the particular solution. (c) (MATLAB) If the car is travelling with constant velocity along a road with rolling hills that can be represented as a cosine function with amplitude Zo and wavelength A (wavelength is the distance between adjacent crests or adjacent troughs, determine the vertical motion of the car as a function of time.

Elements Of Electromagnetics
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3. Quarter car suspension model The figure below a model of the suspension of a car. r(t)is the
position of the mass of the car from its equilibrium position while z is the profile of the road. Note
that z is a function of the distance y along the road, but you need ż(t) which you can obtain from z(y)
using the chain rule. The car is traveling to the right on the road at a speed v. Assume the mass of
the car is 250 kg, the spring constant is 16 kN/m, and damping constant is 1000 Ns/m.
(a) Derive the differential equation for the position of the car r(t).
(b) If z(t) = Zoejot, determine the amplitude and the phase of the particular solution.
(c) (MATLAB) If the car is travelling with constant velocity along a road with rolling hills that
can be represented as a cosine function with amplitude Zo and wavelength A (wavelength is the
distance between adjacent crests or adjacent troughs, determine the vertical motion of the car as
a function of time.
X(t)
Z
m
1
C
Figure 1: Quarter car suspension
(d) (MATLAB) If the car is travelling with constant velocity along a road with road bumps that can
be represented as f(z) = Zol cos woy where y is the distance along the road. Explore this problem
with different wo and Zo.
(e) For both above functions of the road height, do the Fourier series by hand.
Transcribed Image Text:3. Quarter car suspension model The figure below a model of the suspension of a car. r(t)is the position of the mass of the car from its equilibrium position while z is the profile of the road. Note that z is a function of the distance y along the road, but you need ż(t) which you can obtain from z(y) using the chain rule. The car is traveling to the right on the road at a speed v. Assume the mass of the car is 250 kg, the spring constant is 16 kN/m, and damping constant is 1000 Ns/m. (a) Derive the differential equation for the position of the car r(t). (b) If z(t) = Zoejot, determine the amplitude and the phase of the particular solution. (c) (MATLAB) If the car is travelling with constant velocity along a road with rolling hills that can be represented as a cosine function with amplitude Zo and wavelength A (wavelength is the distance between adjacent crests or adjacent troughs, determine the vertical motion of the car as a function of time. X(t) Z m 1 C Figure 1: Quarter car suspension (d) (MATLAB) If the car is travelling with constant velocity along a road with road bumps that can be represented as f(z) = Zol cos woy where y is the distance along the road. Explore this problem with different wo and Zo. (e) For both above functions of the road height, do the Fourier series by hand.
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