1. Physics: Principles with Applications, 6th edition
Lecture PowerPoint
Chapter 11
Physics: Principles with Applications, 6th edition
Giancoli
© 2005 Pearson Prentice Hall
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2. Vibrations and Waves

3. 1 SIMPLE HARMONIC MOTION
Physical Characteristics of Simple Harmonic Oscillators
A mass on a Spring
The Pendulum
Energy in the Simple Harmonic Oscillator
The Period and Sinusoidal Nature of SHM
Oscillations in Electrical Circuits: Similarities in Physics

4. Damped Harmonic Motion
Forced Vibrations; Resonance
Wave Motion
Types of Waves: Transverse and Longitudinal
Energy Transported by Waves
Intensity Related to Amplitude and Frequency
Reflection and Transmission of Waves
Interference; Principle of Superposition
Standing Waves; Resonance
Refraction
Diffraction
Mathematical Representation of a Traveling Wave

5. SIMPLE HARMONIC MOTION
1.1 Physical Characteristics of Simple Harmonic Oscillators
1.2 A Mass on a Spring
1.2.1 A mass on a horizontal spring
1.2.2 A mass on a vertical spring
1.2.3 Displacement, velocity and acceleration in simple harmonic motion
1.2.4 General solutions for simple harmonic motion and the phase angle φ
1.2.5 The energy of a simple harmonic oscillator
1.2.6 The physics of small vibrations
1.3 The Pendulum
1.3.1 The simple pendulum
1.3.2 The energy of a simple pendulum
1.3.3 The physical pendulum
1.3.4 Numerical solution of simple harmonic motion
1.4 Oscillations in Electrical Circuits: Similarities in Physics
1.4.1 The LC circuit
1.4.2 Similarities in physics
PROBLEMS 1

6. Oscillatory Motion
Motion which is periodic in time, that is, motion that repeats itself in time.
Examples:
Power line oscillates when the wind blows past it
Earthquake oscillations move buildings

7. 1 Simple Harmonic Motion
If an object vibrates or oscillates back and forth over the same path, each cycle taking the same amount of time, the motion is called periodic. The mass and spring system is a useful model for a periodic system.

8. 1 Simple Harmonic Motion
We assume that the surface is frictionless. There is a point where the spring is neither stretched nor compressed; this is the equilibrium position. We measure displacement from that point (x = 0 on the previous figure).
The force exerted by the spring depends on the displacement:
(11-1)

9. 1 Simple Harmonic Motion
The minus sign on the force indicates that it is a restoring force – it is directed to restore the mass to its equilibrium position.
k is the spring constant
The force is not constant, so the acceleration is not constant either

10. 1 Simple Harmonic Motion
Displacement is measured from the equilibrium point
Amplitude is the maximum displacement
A cycle is a full to-and-fro motion; this figure shows half a cycle
Period is the time required to complete one cycle
Frequency is the number of cycles completed per second

11. Oscillations of a Spring
Figure Caption: Force on, and velocity of, a mass at different positions of its oscillation cycle on a frictionless surface.

12. Oscillations of a Spring
Displacement is measured from the equilibrium point.
Amplitude is the maximum displacement.
A cycle is a full to-and-fro motion.
Period is the time required to complete one cycle.
Frequency is the number of cycles completed per second.
Figure Caption: Force on, and velocity of, a mass at different positions of its oscillation cycle on a frictionless surface.

13. 11-1 Simple Harmonic Motion
If the spring is hung vertically, the only change is in the equilibrium position, which is at the point where the spring force equals the gravitational force.

15. Oscillations of a Spring
When a family of four with a total mass of 200 kg step into their 1200-kg car, the car’s springs compress 3.0 cm. (a) What is the spring constant of the car’s springs, assuming they act as a single spring? (b) How far will the car lower if loaded with 300 kg rather than 200 kg?
Figure Caption: Photo of a car’s spring. (Also visible is the shock absorber, in blue—see Section 14–7.)
Solution: a. k = F/x = 6.5 x 104 N/m.
b. x = F/k = 4.5 cm

16. Solution:

17. Simple Harmonic Motion
Substituting F = kx into Newton’s second law gives the equation of motion:
with solutions of the form:

18. Simple Harmonic Motion
Substituting, we verify that this solution does indeed satisfy the equation of motion, with:
The constants A and φ will be determined by initial conditions; A is the amplitude, and φ gives the phase of the motion at t = 0.
Figure Caption: Sinusoidal nature of SHM as a function of time. In this case, x = A cos (2πt/T).

19. The velocity can be found by differentiating the displacement:
These figures illustrate the effect of φ:
Figure Caption: Special case of SHM where the mass m starts, at t = 0, at the equilibrium position x = 0 and has initial velocity toward positive values of x (v > 0 at t = 0).
Figure Caption: A plot of x = A cos (ωt +φ) when φ < 0.

20. Simple Harmonic Motion
Because then

21. Simple Harmonic Motion
Determine the period and frequency of a car whose mass is 1400 kg and whose shock absorbers have a spring constant of 6.5 x 104 N/m after hitting a bump. Assume the shock absorbers are poor, so the car really oscillates up and down.
Solution: Substitution gives T = 0.92 s and f = 1.09 Hz.

22. Solution:

23. ω is the angular frequency of the oscillator, with units of rad s-1

24. Figure Caption: Displacement, x, velocity, dx/dt, and acceleration, d2x/dt2, of a simple harmonic oscillator when φ = 0.

25. A is a amplitude: the maximum value of the position of the particle in either the positive or negative x direction.

28. Simple Harmonic Motion
A vibrating floor.
A large motor in a factory causes the floor to vibrate at a frequency of 10 Hz. The amplitude of the floor’s motion near the motor is about 3.0 mm. Estimate the maximum acceleration of the floor near the motor.
Solution: Assuming the motion is simple harmonic, the maximum acceleration is ω2A, where ω = 2πf. This gives a = 12 m/s2.

29. Solution:
Assuming the motion is simple harmonic,

31. The constant angle  is called the phase constant which has units of radians (or initial phase angle) and, along with the amplitude A, is determined uniquely by the position and velocity of the particle at t = 0. If the particle is at its maximum position x = A at t = 0, the phase constant is  = 0 and the graphical representation of the motion is shown in Figure. The quantity (t +) is called the phase of the motion

35. 1 Simple Harmonic Motion
Any vibrating system where the restoring force is proportional to the negative of the displacement is in simple harmonic motion (SHM), and is often called a simple harmonic oscillator.

38. An object oscillates with simple harmonic motion along the x axis
An object oscillates with simple harmonic motion along the x axis. Its position varies with time according to the equation
where t is in seconds and the angles in the parentheses are in radians.
Determine the amplitude, frequency, and period of the motion.
(B) Calculate the velocity and acceleration of the object at any time t.
(C) Using the results of part (B), determine the position,
velocity, and acceleration of the object at t = 1.00 s.
(D) Determine the maximum speed and maximum acceleration of the object
(E) Find the displacement of the object between t =0 and t =1.00 s.

45. Spring calculations.
A spring stretches m when a kg mass is gently attached to it. The spring is then set up horizontally with the kg mass resting on a frictionless table. The mass is pushed so that the spring is compressed m from the equilibrium point, and released from rest. Determine: (a) the spring stiffness constant k and angular frequency ω; (b) the amplitude of the horizontal oscillation A; (c) the magnitude of the maximum velocity vmax; (d) the magnitude of the maximum acceleration amax of the mass; (e) the period T and frequency f; (f) the displacement x as a function of time; and (g) the velocity at t = s.
Solution. A. The spring constant is 19.6 N/m, so ω = 8.08/s−1.
b. Since the spring is released from rest, A = m.
c. The maximum velocity is m/s
d. The maximum acceleration occurs when the displacement is maximum, and equals 6.53 m/s2.
e. The period is s, and the frequency is 1.29 Hz.
f. At t = 0, x = -A; this is a negative cosine. X = (0.100 m)cos (8.08t – π).
g. V = dx/dt; at s it is m/s.

46. Solution:

47. Spring is started with a push.
Suppose the spring of the former example (where ω = 8.08 s-1) is compressed m from equilibrium (x0 = m) but is given a shove to create a velocity in the +x direction of v0 = m/s. Determine (a) the phase angle φ, (b) the amplitude A, and (c) the displacement x as a function of time, x(t).
Solution: a. The tangent of the phase angle is –v0/ωx0 = 0.495, giving φ = 3.60 rad.
b. A = x0/cos φ = m.
c. X = (0.112 m)cos(8.08t )

48. Solution:

50. 1.2.5 The energy of a simple harmonic oscillator

51. 𝟏 𝒅𝒕 = 𝒗 𝒅𝒙
= 𝑚 𝑑𝑣 𝑑𝑡

57. Energy in the Simple Harmonic Oscillator
If the mass is at the limits of its motion, the energy is all potential.
If the mass is at the equilibrium point, the energy is all kinetic.
We know what the potential energy is at the turning points:

58. Energy in the SHO
This graph shows the potential energy function of a spring. The total energy is constant.
Figure Caption: Graph of potential energy, U = ½ kx2. K + U = E = constant for any point x where –A ≤ x ≤ A. Values of K and U are indicated for an arbitrary position x.

59. Energy in the Simple Harmonic Oscillator
The total energy is, therefore
And we can write:
(11-4c)
This can be solved for the velocity as a function of position:
where

61. Energy in the SHO Energy calculations.
For the simple harmonic oscillation where k = 19.6 N/m, A = m, x = -(0.100 m) cos 8.08t, and v = (0.808 m/s) sin 8.08t, determine (a) the total energy, (b) the kinetic and potential energies as a function of time, (c) the velocity when the mass is m from equilibrium, (d) the kinetic and potential energies at half amplitude (x = ± A/2).
Solution: a. E = ½ kA2 = 9.80 x 10-2 J.
b. U = ½ kx2 = (9.80 x 10-2 J) cos2 8.08t, K = ½ mv2 = (9.80 x 10-2 J) sin2 8.08t.
c. v = 0.70 m/s
d. U = 2.5 x 10-2 J, K = E – U = 7.3 x 10-2 J.

62. Solution:

63. Solution:

64. 𝐹 𝑡 =−𝑚g sin𝜃=𝑚 𝑑 2 𝑥 𝑑𝑡 2

65. Energy in the SHO Doubling the amplitude.
Suppose this spring is stretched twice as far (to x = 2A).What happens to (a) the energy of the system, (b) the maximum velocity of the oscillating mass, (c) the maximum acceleration of the mass?
Figure 14-10, repeated.
Solution: a. The total energy is proportional to the square of the amplitude, so it goes up by a factor of 4.
b. The velocity is doubled.
c. The acceleration is doubled.

66. Solution:

67. The Simple Pendulum
In order to be in SHM, the restoring force must be proportional to the negative of the displacement. Here we have:
which is proportional to sin θ and not to θ itself.
However, if the angle is small,
sin θ ≈ θ.

69. The Simple Pendulum Therefore, for small angles, we have: where
The period and frequency are:

71. 𝐾= 1 2 𝑚 𝑣 2 , 𝑈=𝑚𝑔𝑦

77. Oscillations in an LC Circuit

83. When the energy stored in the capacitor has its maximum value, 𝑄 𝑚𝑎𝑥 2 𝐶 , the energy stored in the inductor is zero.
When the energy stored in the inductor has its maximum value, 𝐿 𝐼 𝑚𝑎𝑥 2 , the energy stored in the capacitor is zero.
The sum of the UC + UL is a
constant and equal to the total
energy 𝑄 𝑚𝑎𝑥 2 𝐶 .

84. The kinetic energy of the moving mass, 𝑄 𝑚𝑎𝑥 2 𝐶 is analogous to the energy stored in the inductor, 𝐿 𝐼 𝑚𝑎𝑥 2 , which requires the presence of moving charges.

85. In figure a, all of the energy is stored as electric potential energy in the capacitor at t = 0 s.
In figure b, which is one-fourth of a period later, all of the energy is stored as magnetic energy 𝐿 𝐼 𝑚𝑎𝑥 2 `in the inductor.

86. In figure c, the energy in the LC circuit is stored completely in the capacitor, with the polarity of the plates now opposite to what it was in figure a.
In figure d, all of the energy is stored as magnetic energy 𝐿 𝐼 𝑚𝑎𝑥 2 in the inductor.

87. In figure e, the system has returned to the initial position, completing one oscillation.
At intermediate points, part of the energy is potential energy and part is kinetic energy.
At some time t after the switch is closed and the capacitor has a charge Q and the current is I.
Both the capacitor and the inductor store energy, but the sum of the two energies must equal the total initial energy U stored in the fully charged capacitor at time t = 0 s.

88. Since the circuit resistance is zero, no energy is dissipated as joule heat and the total energy must remain constant over time.
Therefore:
Differentiating the energy equation with respect to time and noting that Q and I vary with time:

90. We can reduce the equation to a differential equation of one variable by using the following relationships:

91. We can solve for the function Q by noting that the equation is of the same form as that of the mass-spring system (simple harmonic oscillator):
where k is the spring constant, m is the mass, and
The solution for the equation has the general form
where ω is the angular frequency of the simple harmonic motion, A is the amplitude of the motion (the maximum value of x), and  is the phase constant; the values of A and  depend on the initial conditions.

92. Writing in the same form as the
differential equation of the simple harmonic oscillator, the solution is:
where Qm is the maximum charge of the capacitor and the angular frequency ω is given by:
The angular frequency of the oscillation depends on the inductance and capacitance of the circuit.
Since Q varies periodically, the current also varies periodically.

93. Differentiating the harmonic oscillator equation for the LC oscillator with respect to time:

94. To determine the value of the phase angle , examine the initial conditions. In the situation presented, when t = 0 s, I = 0 A, and Q = Qm.

95. The time variation of Q and I are given by:
The phase constant  = 0.
The time variation of Q and I are given by:
where Im = ω·Qm is the maximum
current in the circuit.
Graphs of Q vs. t and I vs. t:
The charge on the capacitor
oscillates between the extreme
values Qm and –Qm.

96. Substituting the equations for the oscillating LC circuit into
The current oscillates between
Im and – Im.
The current is 90º out of phase
with the charge.
When the charge reaches an
extreme value, the current is 0;
when the charge is 0, the current
has an extreme value.
Substituting the equations for
the oscillating LC circuit into
the energy equations:

97. Total energy:
The equation shows that the energy of the system continuously oscillates between energy stored in the electric field of the capacitor and energy stored in the magnetic field of the inductor.

98. When the energy stored in the capacitor has its maximum value, , the energy stored in the inductor is zero.
When the energy stored in the inductor has its maximum value, 0.5·L·Im2, the energy stored in the capacitor is zero.
The sum of the UC + UL is a
constant and equal to the total
energy

99. Since the maximum energy stored in the capacitor (when I = 0) must equal the maximum energy stored in the inductor (when Q = 0),
Substituting this into the total energy equation:

100. The total energy U remains constant only if the energy losses are neglected.
In actual circuits, there will always be some resistance and so energy will be lost in the form of heat.
Even when the energy losses due to wire resistance are neglected, energy will also be lost in the form of electromagnetic waves radiated by the circuit.

101. An Oscillatory LC Circuit
An LC circuit has an inductance of 2.81 mH and a capacitance of 9 pF. The capacitor is initially charged with a 12 V battery when the switch S1 is open and switch S2 is closed.
S1 is then closed at the same time
that S2 is opened so that the
capacitor is shorted across the
the inductor.
Find the frequency of the
oscillation.

102. Frequency for an LC circuit:
What are the maximum values of charge on the capacitor and current in the circuit?
Initial charge on the capacitor equals the maximum charge:

103. Maximum current is related to the maximum charge:
Determine the charge and current as functions of time.

104. Energy Oscillations in the LC Circuit and the Mass-Spring System (harmonic oscillator)

107. The Period and Sinusoidal Nature of SHM
Vibration and Waves
The Period and Sinusoidal Nature of SHM

108. The Period and Sinusoidal Nature of SHM
The Period of an object undergoing SHM is independent of the amplitude
Imagine an object traveling in a circular pathway
If we look at the motion in
just the x axis, the
motion is analogous
to SHM

109. The Period and Sinusoidal Nature of SHM
As the ball moves the displacement in the x changes
The radius is the amplitude
The velocity is tangent to the
circle
Now looking at Components
If we put the angles into the
triangle, we can see
similar triangles
Vmax q V A q

110. The Period and Sinusoidal Nature of SHM
So the opposite/hypotenuse is a constant
This can be rewritten
This is the same as the
equation for velocity of
an object in SHM
Vmax q V A q

111. The Period and Sinusoidal Nature of SHM
The period would be the time for one complete revolution
The radius is the same as
the amplitude, and the
time for one revolution
is the period

112. The Period and Sinusoidal Nature of SHM
Using the previous relationship between maximum velocity and amplitude
Substitute in the top equation

113. The Period and Sinusoidal Nature of SHM
Position as a function of time
x displacement is
You don’t know this, but
Where 𝑓 is the frequency So A q

114. The Period and Sinusoidal Nature of SHM
If we look at the projection onto the x axis of an object moving in a circle of radius A at a constant speed vmax, we find that the x component of its velocity varies as:
This is identical to SHM.

115. SHO Related to Uniform Circular Motion
Figure Caption: Analysis of simple harmonic motion as a side view (b) of circular motion (a).

116. The Period and Sinusoidal Nature of SHM
Therefore, we can use the period and frequency of a particle moving in a circle to find the period and frequency:

117. The Period and Sinusoidal Nature of SHM
We can similarly find the position as a function of time:

118. The Period and Sinusoidal Nature of SHM
The top curve is a graph of the previous equation.
The bottom curve is the same, but shifted ¼ period so that it is a sine function rather than a cosine.

119. The Period and Sinusoidal Nature of SHM
The velocity and acceleration can be calculated as functions of time; the results are below, and are plotted at left.