17 : Oscillations Flashcards

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1
Q

oscillating motion

A
  • object starts in equilibrium position a force is applied displacing it and causes it to oscillate
  • it travels towards equilibrium position at and increasing speed it slows down when it goes past equilibrium position eventually reaching max displacement (amplitude) = 0 acceleration and speed
  • max acceleration at equilibrium
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2
Q

displacement

A

the distance from the equilibrium position

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3
Q

amplitude

A

the maximum displacement from the equilibrium position

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4
Q

period

A

the time taken to complete one full oscillation

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5
Q

frequency

A

the number of complete oscillations per unit time

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6
Q

angular frequency

A
  • ω = 2π/T
  • or ω = 2πf
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7
Q

simple harmonic motion

A
  • oscillates either side of a midpoint
  • there is always a restoring force pulling or pushing back towards. the midpoint
  • size of restoring force depends on displacement and force accelerates towards the midpoint
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8
Q

conditions for SMH

A
  • a = ω ^2 x
  • acceleration of the object is directly proportional to its displacement
  • acceleration of object acts opposite direction to the displacement
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9
Q

restoring force

A
  • type of potential force provides restoring ( gpe for pendulums or elastic pe for spring )
  • as objects moves towards the midpoint restoring force does work on object transerferring pe to ke and when moving away from midpoint ke transfers to pe
  • through midpoint pe is zero and ke is max
  • at max displacement ke is zero and pe is max
  • sum of pe and ke = mechanical energy and stays constant
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10
Q

free vibrations

A
  • stretch and release mass on spring it oscillates at is natural frequency
  • if no energy transfers to surroundings it will keep oscillating with the same amplitude forever
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11
Q

forced vibrations

A
  • forced to oscillate by a periodic external force
  • the frequency of this force is called driving frequency
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12
Q

resonance

A
  • when driving frequency approaches natural frequency the system gains more energy from the driving force and vibrates with rapidly increasing amplitude
  • driving frequency = natural frequency
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13
Q

Damping

A
  • any oscillating system loses energy to its surroundings
  • caused usual ly by frictional forces like air resistance
  • systems are deliberately damped to stop them oscillating or to minimise effect of resonance
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14
Q

degree of damping

A
  • damping reduces the amplitude of the oscillation over time
  • critical damping reduces amplitude in the shortest possible time
  • even hever daping are overdamped and take longer to return to equilibrium
  • plastic deformation of ductile materials reduces the amplitude of oscillations in the same way of damping as material changes shape it absorbs energy and oscillation will become smaller
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15
Q

damping affecting resonance

A
  • lightly damped systems have very sharp resonance peak amplitude only increases dramatically when he driving frequency is very close to natural frequency
  • heavily damped systems have a flatter response amplitude doesn’t increase much er natural frequency and aren’t as sensitive to driving frequency
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