Past Paper 2 Flashcards

1
Q

what kind of vehicles would need minimal tyre force and why

A
  • sports and racing cars
  • because road handling, especially around corners, is important
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2
Q

if you had a racing car subjected to large variations of downforce, what would you want to increase about it

A
  • the sprung stiffness
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3
Q

where would a typical car sit on a contoured plot of body acceleration against working space, with contours of spring stiffness and tyre force

A
  • 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
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4
Q

what causes the effect of wheelbase filtering

A
  • 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
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5
Q

explain the mechanism of wheelbase filtering

A
  • 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
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6
Q

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

A
  • 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
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7
Q

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

A
  • undamped: c = 0
  • free vibration: z_r = 0
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8
Q

say you have matrices in the form Mx_dd + Kx = 0. when you take laplace transforms and rearrange it, what is the target expression

A
  • (M^-1K - w^2)x(jw) = 0
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9
Q

how do you finally solve for the natural frequencies with (M^-1K - w^2)x(jw) = 0

A
  • by finding the determinant of the M^-1*K - w^2 matrix
  • keep in mind the diagonal 0s dont get subtracted by w^2
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10
Q

how do you then find the corresponding mode shapes

A
  • 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)
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11
Q

what are the two base expressions for frequency f

A
  • f = v/λ = w/2pi
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12
Q

when doing those very long and scary looking laplace transform questions, what is the key relationship you need to remember to get started

A
  • E[ ] = int[S_y(w) dw = int[ |H_xy(w)|^2*S_x(w)
  • its the linking of two expressions in the datasheet
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13
Q

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

A
  • 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
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14
Q

for the case of roll stiffness T_s = 2k_s*S^2, what is S

A
  • S = T = 0.75m usually
  • unless stated otherwise
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15
Q

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

A
  • 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
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16
Q

what is something unique you have to remember about the unsprung mass roll mode

A
  • because there are two sets of springs in the system
  • you add the suspension roll stiffness T_s and the axle-ground roll stiffness T_t to get total roll stiffness
17
Q

what are the unique things (plural) you have to remember about the sprung mass lateral/roll model

A
  • the sprung mass is drawn like a vertical beam
  • the bottom of it has a horizontal spring attached to a vertical wall on the LHS
  • the middle of it has a curved spring attached to a horizonal wall on the RHS
  • the stiffness of k_lat is so large that it’s assumed to be rigid
  • I in w_n = sqrt(tao/I) is I_s + m(hs - hr)^2, parallel axis theorem
18
Q

for roll-plane analysis, if n_c = 0.2 and U = 30, what does the freuency f equal

A
  • because U = fλ and λ = 1/n, f = Un
  • so 30*0.2 = 6 Hz
19
Q

relating to the expression z_p,dd = z_s,dd + p*θ_s,dd what is the significance of the frequency calculation using f = Un (use the 6 Hz as a frame of ref. for explanation)

A
  • at any given speed, at n_c, the frequency you get determines which mode is primarily expressed
  • when U = 30 so f = 6 Hz, frequencies below 6 Hz has the bounce excitation mainly dominate
  • above 6 Hz, both bounce and roll excitations contribute decent amounts
  • but generally, at high speeds only the bounce modes are excited
20
Q

if the speed U = 1 now, how would that change the ratio of p*θ_s,dd / z_p,dd

A
  • at U = 1, f = 0.2 Hz
  • this means that the bounce and roll motions make similar contributions across the frequency range
  • this shows that, generally, that ratio INCREASES with DECREASING speed
21
Q

what is the approximation of r_2 - r_1 considering their expressions

A
  • r_2 - r_1 = 2yε
22
Q

if you do a question and find that the lateral tracking error y = 0, what suggestion would you give for improving the design of the rigid bogie

A
  • increase the track clearance by 2aθ