this lecture
DESCRIPTION
Driven oscillators Dependence of x on time, t Power. This lecture. x. Solution. t. Transient motion. Steady-state motion. Driven oscillators. Newton equation of motion. Driving force. Method of differentiation and substitution with complex notation to find A 0 and j. - PowerPoint PPT PresentationTRANSCRIPT
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This lecture
Driven oscillators
• Dependence of x on time, t
• Power
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Driven oscillatorsNewton equation of motion
)cos(2 020 t
m
Fxxx
Transientmotion
Steady-statemotion
Solution
t
x)cos(0 tAx
)cos(0 tFF
Driving force
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COMPLEX NOTATION
)cos(0 tAx
)cos(0 tFF
i
mFeAA i
2
/22
0
00
)()(0
titi AeeAx
)(0
tieFF
tiem
Fxxx 02
02
DIFFERENTIATION AND SUBSTITUION gives:
Newton equation in complex form
Method of differentiation and substitution with complex notation complex notation to find to find AA00 and and
*AAA 0
ARe
AImtan
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220 2 res
2220
22
0
0
4 m
F
A
A0
0
Magnitude of displacement x: A0
A0 depends on
A0 has a maximum if 220 2
The frequency corresponding to the maximum of A0 is
220 2res
Increasing damping,
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0 res
2220
22
0
0
4
m
F
A
A0
0
A0has always a maximum
The frequency corresponding to the maximum of A0 is
0 res
Increasing damping,
Magnitude of velocity x: A0
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The frequency at which a relevant parameter becomes maximum is known as the resonance frequency.
Resonance frequency
The sharpness of the resonance curves depends on the strength of damping (). In the limit , both displacement and velocity tend to infinity.
Two resonance frequencies
for the displacement
for the velocity
The two values are equal if
220 2 res
0 res
0
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Phase of displacement,
Displacement and force are out of phase
)cos(0 tAx)cos(0 tFF
depends on
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Phase of displacement,
20
2
2
tan
])[()(
/
imF
A 24
22022222
0
0
sincos 000 iAAeAA i
The displacement always lags the force
A
A
Re
Imtan
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Phase of velocity, *
At resonance the velocity is in phase
with the force
)cos( tAx 0
)cos()sin(200
tAtAx
2
**)cos( tAx 0
0
)cos(
)cos(
tFF
tAx
0
0
)cos( tFF 0
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“Sloshing” of waterFind the resonance frequency in the
absence of damping
ExamplesLakesTea-cup Bathtub…
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“Sloshing” of water• In the absence of damping the resonance frequency res
is equal to the natural frequency 0
• Natural frequency 0
2R
R
Axis of rotation
• 0 = natural frequency of a physical pendulum
I
mgd0
d = distance of the centre of mass from axis of rotation
m = mass of water I = momentum of inertia
d
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“Sloshing” of water Natural frequency 0
2R
d
R
g
R
g
I
mgd~
3
80
3
4Rd
2
2
1mRI
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“Sloshing” of water
L
h
Consider general geometry
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Lock Ness monster or a sloshing mode?
R
g~0
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Power Power The oscillator absorbs more energy
when the frequency of the driving force, , matches the natural frequency,
0
Po
we
r, P
Driving frequency,
increasingdamping
Light,
Atom,
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Power Power The oscillator absorbs more energy
when the frequency of the driving force, , matches the natural frequency,
Light,
Atom,
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Power Power The oscillator absorbs more energy
when the frequency of the driving force, , matches the natural frequency,
0
Po
we
r, P
Driving frequency,
increasingdamping