Past Paper 2 Flashcards
what kind of vehicles would need minimal tyre force and why
- sports and racing cars
- because road handling, especially around corners, is important
if you had a racing car subjected to large variations of downforce, what would you want to increase about it
- the sprung stiffness
where would a typical car sit on a contoured plot of body acceleration against working space, with contours of spring stiffness and tyre force
- the main point is that the spring stiffness would be between 20 and 30 kN/m
- the damping would be around 2-3kNs/m for extra info
what causes the effect of wheelbase filtering
- the time delay between the road input to the front and rear axles
- this results in multiple peaks and troughs in the transfer function of the two DOF pitch-plane model
explain the mechanism of wheelbase filtering
- consider a massless, suspensionless vehicle with wheelbase L
- the wheelbase travels along a sinusoidal profile with wavelength λ
- the wheelbase filters out pitch excitation when L = Nλ and N is an integer
- the wheelbase filters out bounce excitation when L = (N+0.5)λ and N is an integer
- filtering out the excitation means that their respective gains are 0
what is the expression for the natural frequency of the bounce mode f_bounce and pitch mode f_pitch if the excitation of the mode is minimized
- f = U/λ in general
- wheelbase filters out bounce excitation when L = (N+0.5)λ
- so f_bounce = U(N+0.5) / L
- wheelbase filters out pitch excitation when L = Nλ
- so f_pitch = UN / L
when trying to find the natural frequencies of a system, you want the natural modes of vibration. what are the two conditions for natural modes
- undamped: c = 0
- free vibration: z_r = 0
say you have matrices in the form Mx_dd + Kx = 0. when you take laplace transforms and rearrange it, what is the target expression
- (M^-1K - w^2)x(jw) = 0
how do you finally solve for the natural frequencies with (M^-1K - w^2)x(jw) = 0
- by finding the determinant of the M^-1*K - w^2 matrix
- keep in mind the diagonal 0s dont get subtracted by w^2
how do you then find the corresponding mode shapes
- by finding the eigenvectors of the matrix for each natural frequency
- input the frequency, and the matrix multiplied by the main variables matrix = 0
- then figure out what has to be 0 and what can be 1 (usually 1)
what are the two base expressions for frequency f
- f = v/λ = w/2pi
when doing those very long and scary looking laplace transform questions, what is the key relationship you need to remember to get started
- E[ ] = int[S_y(w) dw = int[ |H_xy(w)|^2*S_x(w)
- its the linking of two expressions in the datasheet
in the case of roll-plane analysis, what does it suggest if youre told to find the natural frequencies and mode shapes at low speeds
- that y_dot is small so the dampers can be ignored
- so when you draw the simplified versions of the 6 DOF model you dont include the damper in between the sprung and unsprung masses
for the case of roll stiffness T_s = 2k_s*S^2, what is S
- S = T = 0.75m usually
- unless stated otherwise
when finding the natural frequencies in the roll-plane analysis, being told that the speed is low so dampers can be ignored, you can draw 4 modes (sprung mass vertical, unsprung mass vertical, unpsprung mass roll and sprung mass lateral+roll). what are the general expressions for the natural frequencies youll be using in these cases
- for the vertical modes, w_n = sqrt(k/m)
- for the roll and lateral modes, w_n = sqrt(tao/I)
- tao are the roll stiffness equations
- I is the moment of inertia