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4.5 Earth's Gravitational Field ( examples )
Action at a distance, effect of a body A exerting a force on another body B. Due to a gravitational field around A.
Gravitational field strength, ____g =
=
_______
___Variation of g with height.
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4.6 Artificial Satellites ( examples )
_______
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4.7 Escape Speed ( examples )
___
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4.8 Weightlessness In Orbit ( examples )
When Fc = Fg \ no net force experienced in ship, no net acceleration relative to ship
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For a body in a lift descending___ mg - S = ma___ if S = mg Þ weightlessness ( S is normal reaction )
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4.9 Simple Harmonic Motion ( examples )
In oscillatory motion the acceleration, displacement & velocities change periodically (in magnitude & direction).
Definition of SHM - If the acceleration of a body is directly proportional to its distance from a fixed point and is always directed towards that point, the motion is simple harmonic.
__________________________
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4.10 Equations of SHM ( examples )
Time peiod , T - time to complete one cycle or oscillation.
Frequency, f - number of oscillations per second.
Amplitude, A or r - maximum displacement from mean position.
Phase, f - the initial angular state of the system, usually as a fraction of the time period.
Phase difference, Df degree to which oscillations are out of step, in relation to the time interval between maximum displacements._______Df = (time difference at maximas) / (time period)
acceleration,_a µ - x,_______a = - k x = - w x2 = - w2A sin wt,____ velocity,_v = - vm cos wt = w ± ( A2 - x2 )½
max. velocity, vm = ± wA____displacement,_x = A sin wt = A sin ( wt + f )__if x = 0 at t = 0 then f = 0,
(q = wt, vm = wA ), __T =
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4.11 Mass on a Spring ( examples )
_______________________________
Hooke's law :________T = ke, \ T0 = mg = ke0 ( equilibrium )
When displaced, x : ___F = mg - T = mg - k ( e0 + x ) = mg - mg - kx
Newton's 2nd law : ___.F = ma, \ ma = - kx \ a =
\ period T = 2p
SHM Experiment to find 'g' using mass on a spring
_____
From (4.11): T2 = 4p2
and
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4.12 Simple Pendulum ( examples )
for x & q small ® sin q =
Force towards centre (
to tension ), F = - mg
_____
T =
SHM Experiment to find 'g' using a pendulum
F = mg
____
acc. = - wx2 = g
____
Þ w2 =
____\ w =
As T =
____then T2 =
If g = 9.8 ms- 2 then the experiment has accurately been measured for SHM where acc. = - wx2 .
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4.13 Energy of SHM ( examples )
PE = ½ F x____( F = k x )____\ PE = ½ k x2 = ½ m w2y2 ____(amplitude a2 = x2 + y2, y can be incorporated into diagram 4.9)
KE = ½ m v2 = ½ m w2x2____E = KE + PE__ (conservation of mechanical energy)
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4.14 Damped Oscillations ( examples )
Damping :
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4.15 Forced Oscillations and Resonance ( examples )
The graph relates to the experiment with 'Bartons pendulum' & also other SHM systems.
____
Examples of resonance Þ air column in musical instrument, radio tuned to natural frequency = radio signal (electrical resonance), Tacoma Narrows Bridge disaster - wind caused oscillating force in resonance with natural frequency of the bridge.
Experiment to find resonant amplitude - Barton's pendulums
Frequency, f, found from time exposure photographs. Resonant pendulum = 1/4 oscillation behind diver pendulum.
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Reference
1. If s = r then q = 1 radian ( rad ) - 1 rad is the angle subtended at the centre of a circle by an arc = in length to the radius. The circumference is s = 2pr where q = 2p rad. ( or 360° )
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Page Last Updated: November 2005