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PHYSICS 231 INTRODUCTORY PHYSICS I
Lecture 21
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Last Lecture Simple Harmonic Motion
, f, T determined by mass and spring constant A, determined by initial conditions: x(0), v(0)
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Example 13.3 A 36-kg block is attached to a spring of constant k=600 N/m. The block is pulled 3.5 cm away from its equilibrium position and is pushed so that is has an initial velocity of 5.0 cm/s at t=0. a) What is the position of the block at t=0.75 seconds? a) cm
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Example 13.4a An object undergoing simple harmonic motion follows the expression, Where x will be in cm if t is in seconds The amplitude of the motion is: a) 1 cm b) 2 cm c) 3 cm d) 4 cm e) -4 cm
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Example 13.4b An object undergoing simple harmonic motion follows the expression, Here, x will be in cm if t is in seconds The period of the motion is: a) 1/3 s b) 1/2 s c) 1 s d) 2 s e) 2/ s
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Example 13.4c An object undergoing simple harmonic motion follows the expression, Here, x will be in cm if t is in seconds The frequency of the motion is: a) 1/3 Hz b) 1/2 Hz c) 1 Hz d) 2 Hz e) Hz
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Example 13.4d An object undergoing simple harmonic motion follows the expression, Here, x will be in cm if t is in seconds The angular frequency of the motion is: a) 1/3 rad/s b) 1/2 rad/s c) 1 rad/s d) 2 rad/s e) rad/s
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Example 13.4e An object undergoing simple harmonic motion follows the expression, Here, x will be in cm if t is in seconds The object will pass through the equilibrium position at the times, t = _____ seconds a) …, -2, -1, 0, 1, 2 … b) …, -1.5, -0.5, 0.5, 1.5, 2.5, … c) …, -1.5, -1, -0.5, 0, 0.5, 1.0, 1.5, … d) …, -4, -2, 0, 2, 4, … e) …, -2.5, -0.5, 1.5, 3.5,
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Simple Pendulum Looks like Hooke’s law (k mg/L)
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Simple Pendulum
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Frequency independent of mass and amplitude! (for small amplitudes)
Simple pendulum Frequency independent of mass and amplitude! (for small amplitudes)
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Pendulum Demo
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Example 13.5 A man enters a tall tower, needing to know its height h. He notes that a long pendulum extends from the roof almost to the ground and that its period is 15.5 s. (a) How tall is the tower? (b) If this pendulum is taken to the Moon, where the free-fall acceleration is 1.67 m/s2, what is the period of the pendulum there? a) 59.7 m b) 37.6 s
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Damped Oscillations In real systems, friction slows motion
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TRAVELING WAVES Sound Surface of a liquid Vibration of strings
Electromagnetic Radio waves Microwaves Infrared Visible Ultraviolet X-rays Gamma-rays Gravity
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Longitudinal (Compression) Waves
Elements move parallel to wave motion. Example - Sound waves
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Transverse Waves Elements move perpendicular to wave motion.
Examples - strings, light waves
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Compression and Transverse Waves Demo
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Snapshot of a Transverse Wave
wavelength x
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Snapshot of Longitudinal Wave
y could refer to pressure or density
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Moving Wave Replace x with x-vt if wave moves to the right. Replace with x+vt if wave should move to left. moves to right with velocity v Fixing x=0,
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Moving Wave: Formula Summary
- moving to right + moving to left
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Example 13.6a A wave traveling in the positive x direction has a frequency of f = 25.0 Hz as shown in the figure. The wavelength is: a) 5 cm b) 9 cm c) 10 cm d) 18 cm e) 20 cm
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Example 13.6b A wave traveling in the positive x direction has a frequency of f = 25.0 Hz as shown in the figure. The amplitude is: a) 5 cm b) 9 cm c) 10 cm d) 18 cm e) 20 cm
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Example 13.6c A wave traveling in the positive x direction has a frequency of f = 25.0 Hz as shown in the figure. The speed of the wave is: a) 25 cm/s b) 50 cm/s c) 100 cm/s d) 250 cm/s e) 500 cm/s
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Example 13.7a Consider the following expression for a pressure wave, where it is assumed that x is in cm,t is in seconds and P will be given in N/m2. What is the amplitude? a) 1.5 N/m2 b) 3 N/m2 c) 30 N/m2 d) 60 N/m2 e) 120 N/m2
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Example 13.7b Consider the following expression for a pressure wave, where it is assumed that x is in cm,t is in seconds and P will be given in N/m2. What is the wavelength? a) 0.5 cm b) 1 cm c) 1.5 cm d) cm e) 2 cm
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Example 13.7c Consider the following expression for a pressure wave, where it is assumed that x is in cm,t is in seconds and P will be given in N/m2. What is the frequency? a) 1.5 Hz b) 3 Hz c) 3/ Hz d) 3/(2) Hz e) 3 Hz
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Example 13.7d Consider the following expression for a pressure wave, where it is assumed that x is in cm,t is in seconds and P will be given in N/m2. What is the speed of the wave? a) 1.5 cm/s b) 6 cm/s c) 2/3 cm/s d) 3/2 cm/s e) 2/ cm/s
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Example 13.8 Which of these waves move in the positive x direction?
a) 5 and 6 b) 1 and 4 c) 5,6,7 and 8 d) 1,4,5 and 8 e) 2,3,6 and 7
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Speed of a Wave in a Vibrating String
For other kinds of waves: (e.g. sound) Always a square root Numerator related to restoring force Denominator is some sort of mass density
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Example 13.9 A string is tied tightly between points A and B as a communication device. If one wants to double the wave speed, one could: a) Double the tension b) Quadruple the tension c) Use a string with half the mass d) Use a string with double the mass e) Use a string with quadruple the mass
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Superposition Principle
Traveling waves can pass through each other without being altered.
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Reflection – Fixed End Reflected wave is inverted
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Reflection – Free End Reflected pulse not inverted
Vibrations and Waves Honors Physics.
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Chapter 13 Vibrations and Waves. When x is positive, F is negative ; When at equilibrium (x=0), F = 0 ; When x is negative, F is positive ; Hooke’s Law.
Chapter 13 VibrationsandWaves. Hooke’s Law F s = - k x F s = - k x F s is the spring force F s is the spring force k is the spring constant k is the spring.
Chapter 13 Vibrations and Waves. When x is positive, F is negative ; When at equilibrium (x=0), F = 0 ; When x is negative, F is positive ; Hooke’s.
Oscillations 1. Different types of motion: Uniform motion 1D motion with constant acceleration Projectile motion Circular motion Oscillations 2. Different.
Chapter 13 Vibrations and Waves.
Vibrations and Waves Chapter 12.
Simple Harmonic Motion
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Vibrations and Waves Chapter 11.
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Holt Physics Chapter 11 Vibrations and Waves Simple Harmonic Motion Simple Harmonic Motion – vibration about an equilibrium position in which a restoring.
Chapter 13 Vibrations and Waves. Hooke’s Law F s = - k x F s is the spring force k is the spring constant It is a measure of the stiffness of the spring.
Vibrations and Waves Chapter 12.
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