Vehicle Vibration 2 Flashcards

1
Q

what are the three important performance criteria of a vehicle

A
  • body acceleration
  • working space
  • dynamic tyre force
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2
Q

what is the rms body acceleration

A
  • rms body acceleration = sqrt(E[z_doubledot_s^2])
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3
Q

what is the rms working space

A
  • rms working space = sqrt(E[(z_s - z_u)^2])
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4
Q

what is the rms tyre force

A
  • rms tyre force = sqrt(E[(k_t*(z_r - z_u))^2])
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5
Q

for pitch-plane analysis, what is the general equation of motion in matrix-vector notation

A
  • Mx_dotdot + Cx_dot + Kx = Pu_dot + R*u
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6
Q

if you are operating under natural modes of vibration, meaning stiffnesses c_1 = c_2 = 0 and the displacements z_r1 = z_r2 = 0, how would you find a solution to the equation of motion

A
  • take laplace transforms to get: M^-1Kx(jw) = w^2x(jw)
  • solutions are the e-values and e-vectors of M^-1*K
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7
Q

in the special case of uncoupled equations where k_1a = k_2b, what is the frequency w^2 in pure bounce mode

A
  • w^2 = k_1 + k_2 / m
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8
Q

in the special case of uncoupled equations where k_1a = k_2b, what is the frequency w^2 in pure pitch mode

A
  • w^2 = k_1a^2 + k_2b^2 / I
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9
Q

what is z_r2(t) in terms of z_r1(t) where a is the distance between G and z_r1 at the front while b is the distance between G an z_r2 in the back

A
  • z_r2(t) = z_r1(t)*(t - (a+b)/V)
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10
Q

what is the wavenumber n

A
  • n = 1/λ = w/2pi*V
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11
Q

what is the normalised wavenumber N

A
  • N = L/λ = L*n
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12
Q

what is the magnitude for the bounce gain

A
  • bounce gain = sqrt(1+cos(2pi*N) / 2)
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13
Q

what is the magnitude for pitch gain

A
  • pitch gain = sqrt(1-cos(2pi*N) / 2)
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14
Q

what is the body acceleration physically

A
  • it is the acceleration of the sprung mass
  • it is a proxy for discomfort in a vehicle
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15
Q

what is the working space physically

A
  • the space available for relative displacement of the sprung and unsprung masses
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16
Q

what is the tyre force physically

A
  • the ability of the tyres to generate breaking or cornering force
  • this is reduced if the vertical tyre force oscillates
17
Q

relating to contours of RMS body acceleration, when is body acceleration minimized

A
  • when k and c are 0
18
Q

what happens to the RMS body acceleration if damping is small but stiffness is not

A
  • large values of acceleration occur
19
Q

relating to contours of RMS working space, what does it rely on wrt to damping and stiffness

A
  • only damping
  • working space increases as damping decreases
20
Q

what is the relationship between RMS working space and damping if suspension is locked

A
  • damping is infinite
  • so working space is 0
21
Q

relating to contours of RMS tyre force, when is it minimized

A
  • at a specific combination of non-zero damping and stiffness
  • because the contours are circular