SHM/Circular motion

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26 Terms

1
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Significance of banked tracks

Horizontal component of the normal contact force, which provides extra centripetal force

Enables objects to complete circle at greater speed without skidding

2
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Banked tracks equation

v² = rgtantheta

No friction

Where r is radius of circle, g acceleration due to gravity, theta slope of angle

3
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Define shm

The relationship between the acceleration of an object and it's displacement

4
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Conditions for shm

Acceleration is directly proportional to displacement

Acceleration is in the opposite direction to displacement

5
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Features of time period in shm

Independent of amplitude

Increases as mass increases but not directly proportional

6
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Amplitude definition

Maximum displacement from equilibrium position

7
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When does maximum speed occur

When an object passes through the equilibrium position

8
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When does maximum acceleration occur

At the extremes of the oscillation

9
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For pendulum shim restoring force

F = mgsintheta. = mgtheta small angle approximation

10
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Free oscillation definition

Energy is conserved (no friction) so amplitude is constant

11
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Damped oscillation definition

Energy is lost to their surroundings due to friction, air resistance, etc.

12
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Damping definition

Resistive force which acts in the opposite direction to velocity to reduce amplitude

13
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Natural frequency definition

Frequency the system oscillates at with no energy input

14
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Forced vibration

Oscillation caused by a periodic driving force

15
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Free vibration

When a system is displaced and left to oscillate

16
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Resonance

Occurs when driving oscillation is at the same frequency as the natural frequency

Leads to sharp increase in amplitude = large amplitude

17
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When forced frequency ≠ natural frequency

Forced vibration at given frequency and small amplitude

18
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The effect of damping on resonance

No/little damping, largest value for max amplitude occurs when frequency driving oscillation = natural frequency

Resonant frequency decreases as the degree of damping increases

The resonance curve becomes less sharp as the damping is increased

19
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Phase difference for driving frequency much less than natural frequency

Phase difference = 0

Amplitude ≈ of applied

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Phase difference for driving frequency = natural f

Phase difference = 90

21
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Phase difference for driving f much larger than natural f

Phase difference = 180

22
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Reducing effects of resonance

Extra damping to absorb energy and reduce amplitude

Change natural frequency (e.g. adding mass)

23
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Light damping

Takes a long time for the amplitude to decrease to 0. System oscillates at natural f

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Critical damping

Shortest time for amplitude to decrease to 0

25
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Heavy damping

Takes long time for amplitude to decrease to 0. No oscillating motion occurs

26
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Conditions in time period equation of a pendulum

Oscillations with a small amplitude

Angular displacement <10°