Module 3 Flashcards

1
Q

types of loading considered harmonic

A
  • structures supporting vibrating machines
  • certain types of wind loading
  • pedestrian loading
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2
Q

applied force of harmonic vibration

A

p(0)sinwt
where
p(0) is the amplitude of the force
w is the excitation frequency

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3
Q

two parts to harmonic excitation solution

A
  • steady state component

- transient solution

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4
Q

steady state solution (undamped)

A

particular solution

- represents oscillation at the frequency of the forcing function w

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5
Q

transient solution (undamped)

A

complimentary solution

- represents oscillation at the natural frequency of the SDOF, w(n)

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6
Q

what happens when introduce damping to harmonic loading

A

transient solution dies away over time and total displacement tends toward steady state solution

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7
Q

Special case

A

RESONANCE

w = w(n)

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8
Q

transient response (damped)

A

oscillates at damped natural frequency, w(d)

- term decays in amplitude over time

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9
Q

steady state response (damped)

A

oscillates at excitation frequency, w

- does not decay with time

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10
Q

speed with which transient response decays

A

is a function of the damping ratio

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11
Q

for a given w/w(n) what happens as damping ratio is decreased

A

Rd increases

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12
Q

at very small w/w(n)

A

dynamic response amplitude effectively the same as static response

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13
Q

at very large w / w(n)

A

dynamic response tends to zero (very flexible structure)

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14
Q

max Rd

A

doesnt always occur at w / w(n) = 1

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15
Q

special case at w / w(n) = 1

A

always has a phase lag of 90 degrees, regardless of damping ratio

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16
Q

small damping ratio at w / w(n) = 1

A

causes rapid change in phase lag

17
Q

vibration generators

A

work by having two masses rotating in opposite directions about a vertical axis
- mass of vibration generator small compared to structure

18
Q

vibration generator exciting force

A

p(t) = (m(e) e w^2) sinwt

19
Q

fT

A

force transmitted to supports of system

fT = fs + fD

20
Q

TR

A

transmissibility

TR = fT,max / p(0)

21
Q

effect of damping on transmitted force

A
  • increased damping decreases transmitted force for frequency ratios less than sqrt(2)
  • increases transmitted force for w/w(n) > sqrt(2) so ideally no damping then
22
Q

natural frequency so that transmitted force is less than applied force

A

w / w(n) > sqrt(2) by having a small enough w(n)

23
Q

trade off with damping and transmitted force

A

for w / w(n) > sqrt(2)

trade off between soft spring to reduce transmitted force and an acceptable static displacement