lecture 11: simple harmonic motionzimp.zju.edu.cn/~xinwan/courses/physi17/handouts/lecture11.pdf ·...
TRANSCRIPT
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General Physics IGeneral Physics I
Lecture 11: Simple Harmonic Lecture 11: Simple Harmonic MotionMotion
Prof. WAN, Xin (万歆)
[email protected]://zimp.zju.edu.cn/~xinwan/
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OutlineOutline
● The conditions for static equilibrium ● Motion near the stable equilibrium● Simple harmonic motion● The block-spring system in quantitative treatment● Energy of the simple harmonic oscillator
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● The necessary condition for equilibrium is that the net force acting on an object be zero.
For Point-like ObjectsFor Point-like Objects
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For Extended ObjectsFor Extended Objects
● A second condition is that the net torque about any axis be zero.
● The two conditions are the statements of
− Translational equilibrium− Rotational equilibrium
Not in equilibrium!
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Static EquilibriumStatic Equilibrium
● An object is in equilibrium means that both the linear acceleration and the angular acceleration are zero.
● If the object is at rest and so has no linear speed or angular speed, the object is in static equilibrium.
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TorqueTorque
● The torque t involves the two vectors r and F, and its direction is perpendicular to the plane of r and F. We can establish a mathematical relationship between t, r, and F, using a new mathematical operation called the vector product, or cross product
Will discuss more next week.
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Torque about Any Point?Torque about Any Point?
If an object is in translational equilibrium and the net torque is zero about one point, then the net torque must be zero about any other point.
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Center of GravityCenter of Gravity
To compute the torque due to the gravitational force on an object of mass M, we need only consider the force Mg acting at the center of gravity of the object.
The center of gravity is located at the center of mass as long as the object is in a uniform gravitational field.
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Example: A Weighted HandExample: A Weighted Hand
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Example: Standing on a BeamExample: Standing on a Beam
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Example: The Leaning LadderExample: The Leaning Ladder
Find the minimum angle at which the ladder does not slip.
Take the torques about an axis through the origin O at the bottom of the ladder
Because the ladder is stationary, the three forces acting on it must all pass through some common point.
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Example: Up the CurbExample: Up the Curb
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Equilibrium of a SystemEquilibrium of a System
In general, positions of stable equilibrium correspond to points for which U(x) is a minimum.
dUdx
=0d2Udx2 >0
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Elastic Potential EnergyElastic Potential Energy
● The elastic potential energy of the system can be thought of as the energy stored in the deformed spring (one that is either compressed or stretched from its equilibrium position).
W s = ∫xi
x f
(−kx)dx =12kxi
2−12kx f
2
= U i−U f
= −(U f−U i) = −ΔUg
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Elastic Potential EnergyElastic Potential Energy
● The elastic potential energy associated with the system is defined by
F = −kx = −dUdx
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Motion near Stable EquilibriumMotion near Stable Equilibrium
Positions of stable equilibrium correspond to points for which U(x) is a minimum.
dUdx
= 0
d2Udx2 > 0
U(x)
x
Equilibrium (F = 0)
Stable
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Taylor ExpansionTaylor Expansion
● We can Taylor expand the potential energy near the equilibrium
● Quite generically, we expect linear restoring force like in the block-spring system, if we neglect the higher order terms (which are usually small if we stay close enough to the equilibrium).
● This universal family of motion is known as the simple harmonic motion.
U (x) = U (x0) +dUdx ∣
x=x0
(x−x0) +12d2Udx2 ∣
x=x0
(x−x0)2
+ ⋯
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Simple Harmonic MotionSimple Harmonic Motion
● An object moves with simple harmonic motion whenever its acceleration is proportional to its displacement from some equilibrium position and is oppositely directed.
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Quantitative AnalysisQuantitative Analysis
Define
Solution:
Please check that the differential equation is satisfied.
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The Meaning of the SolutionThe Meaning of the Solution
A: Amplitude of the oscillation
T = 2p / w : Period of the oscillation
f : Phase constant, or phase angle
Understand how to draw the x-t curve, and how to read information from the x-t curve.
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Period and FrequencyPeriod and Frequency
● The period T of the motion is the time it takes for the particle to go through one full cycle.
● The frequency represents the number of oscillations that the particle makes per unit time.
Angular frequency:
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Not in PhaseNot in Phase
p/2 out of phase with the displacement
p out of phase with the displacement
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Important ObservationsImportant Observations
● The acceleration of the particle is proportional to the displacement but is in the opposite direction. This is the necessary and sufficient condition for simple harmonic motion, as opposed to all other kinds of vibration.
● The displacement from the equilibrium position, velocity, and acceleration all vary sinusoidally with time but are not in phase.
● The frequency and the period of the motion are independent of the amplitude.
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Energy of the Harmonic OscillatorEnergy of the Harmonic Oscillator
The total mechanical energy of a simple harmonic oscillator is a constant of the motion and is proportional to the square of the amplitude.
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Energy TransformEnergy Transform