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Chapter 13 VibrationsandWaves. Hookes Law 13.1 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.

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Presentation on theme: "Chapter 13 VibrationsandWaves. Hookes Law 13.1 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."— Presentation transcript:

1 Chapter 13 VibrationsandWaves

2 Hookes Law 13.1 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 constant It is a measure of the stiffness of the spring It is a measure of the stiffness of the spring –A large k indicates a stiff spring and a small k indicates a soft spring x is the displacement of the object from its equilibrium position x is the displacement of the object from its equilibrium position The negative sign indicates that the force is always directed opposite to the displacement The negative sign indicates that the force is always directed opposite to the displacement

3 Hookes Law Force The force always acts toward the equilibrium position The force always acts toward the equilibrium position It is called the restoring force It is called the restoring force The direction of the restoring force is such that the object is being either pushed or pulled toward the equilibrium position The direction of the restoring force is such that the object is being either pushed or pulled toward the equilibrium position

4 Hookes Law Applied to a Spring – Mass System When x is positive (to the right), F is negative (to the left) When x is positive (to the right), F is negative (to the left) When x = 0 (at equilibrium), F is 0 When x = 0 (at equilibrium), F is 0 When x is negative (to the left), F is positive (to the right) When x is negative (to the left), F is positive (to the right)

5 Motion of the Spring-Mass System Assume the object is initially pulled to x = A and released from rest Assume the object is initially pulled to x = A and released from rest As the object moves toward the equilibrium position, F and a decrease, but v increases As the object moves toward the equilibrium position, F and a decrease, but v increases At x = 0, F and a are zero, but v is a maximum At x = 0, F and a are zero, but v is a maximum The objects momentum causes it to overshoot the equilibrium position The objects momentum causes it to overshoot the equilibrium position The force and acceleration start to increase in the opposite direction and velocity decreases The force and acceleration start to increase in the opposite direction and velocity decreases The motion continues indefinitely The motion continues indefinitely

6 Simple Harmonic Motion Motion that occurs when the net force along the direction of motion is a Hookes Law type of force Motion that occurs when the net force along the direction of motion is a Hookes Law type of force The force is proportional to the displacement and in the opposite direction The force is proportional to the displacement and in the opposite direction The motion of a spring mass system is an example of Simple Harmonic Motion The motion of a spring mass system is an example of Simple Harmonic Motion

7 Simple Harmonic Motion, cont. Not all periodic motion over the same path can be considered Simple Harmonic motion Not all periodic motion over the same path can be considered Simple Harmonic motion To be Simple Harmonic motion, the force needs to obey Hookes Law To be Simple Harmonic motion, the force needs to obey Hookes Law

8 Amplitude Amplitude, A Amplitude, A The amplitude is the maximum position of the object relative to the equilibrium position The amplitude is the maximum position of the object relative to the equilibrium position In the absence of friction, an object in simple harmonic motion will oscillate between ±A on each side of the equilibrium position In the absence of friction, an object in simple harmonic motion will oscillate between ±A on each side of the equilibrium position

9 Period and Frequency The period, T, is the time that it takes for the object to complete one complete cycle of motion The period, T, is the time that it takes for the object to complete one complete cycle of motion From x = A to x = - A and back to x = A From x = A to x = - A and back to x = A The frequency, ƒ, is the number of complete cycles or vibrations per unit time The frequency, ƒ, is the number of complete cycles or vibrations per unit time

10 Acceleration of an Object in Simple Harmonic Motion Newtons second law will relate force and acceleration Newtons second law will relate force and acceleration The force is given by Hookes Law The force is given by Hookes Law F = - k x = m a F = - k x = m a a = -kx / m a = -kx / m The acceleration is a function of position The acceleration is a function of position Acceleration is not constant and therefore the uniformly accelerated motion equation cannot be applied Acceleration is not constant and therefore the uniformly accelerated motion equation cannot be applied

11 Sample problem 13.1 A spring with constant k=475 N/m stretch 4.50 cm when an object of mass 25.0 kg is attached to the end of the spring. Find the acceleration of gravity in this location. (0.855 m/s 2 )

12 Sample Problem 13.2 A kg object attached to a spring of force constant 130 N/m is free to move on a frictionless horizontal surface. If the object is released from rest at x = m find the force and acceleration of the object. (Ans: -13 N; -37 m/s 2 ) A kg object attached to a spring of force constant 130 N/m is free to move on a frictionless horizontal surface. If the object is released from rest at x = m find the force and acceleration of the object. (Ans: -13 N; -37 m/s 2 )

13 Acceleration Defining Simple Harmonic Motion Acceleration can be used to define simple harmonic motion Acceleration can be used to define simple harmonic motion An object moves in simple harmonic motion if its acceleration is directly proportional to the displacement and is in the opposite direction An object moves in simple harmonic motion if its acceleration is directly proportional to the displacement and is in the opposite direction

14 Elastic Potential Energy 13.2 A compressed spring has potential energy A compressed spring has potential energy The compressed spring, when allowed to expand, can apply a force to an object The compressed spring, when allowed to expand, can apply a force to an object The potential energy of the spring can be transformed into kinetic energy of the object The potential energy of the spring can be transformed into kinetic energy of the object

15 Elastic Potential Energy, cont The energy stored in a stretched or compressed spring or other elastic material is called elastic potential energy The energy stored in a stretched or compressed spring or other elastic material is called elastic potential energy Pe s = ½kx 2 Pe s = ½kx 2 The energy is stored only when the spring is stretched or compressed The energy is stored only when the spring is stretched or compressed Elastic potential energy can be added to the statements of Conservation of Energy and Work-Energy Elastic potential energy can be added to the statements of Conservation of Energy and Work-Energy

16 Energy in a Spring Mass System A block sliding on a frictionless system collides with a light spring A block sliding on a frictionless system collides with a light spring The block attaches to the spring The block attaches to the spring

17 Energy Transformations The block is moving on a frictionless surface The total mechanical energy of the system is the kinetic energy of the block

18 Energy Transformations, 2 The spring is partially compressed The energy is shared between kinetic energy and elastic potential energy The total mechanical energy is the sum of the kinetic energy and the elastic potential energy

19 Energy Transformations, 3 The spring is now fully compressed The block momentarily stops The total mechanical energy is stored as elastic potential energy of the spring

20 Energy Transformations, 4 When the block leaves the spring, the total mechanical energy is in the kinetic energy of the block The spring force is conservative and the total energy of the system remains constant

21 Sample problem 13.3 A 13,000 N car starts at rest and rolls down a hill from a height of 10.0 m. I then moves across a level surface and collides with a light spring-loaded guardrail. A) neglecting friction, what is the maximum distance the spring is compressed if the spring constant is 1.0 x 106 N/m. B) Calculate the max. acceleration of the car after contact with the spring, again neglect friction. C) if the spring is compressed by only 0.30 m, find the energy lost through friction. A 13,000 N car starts at rest and rolls down a hill from a height of 10.0 m. I then moves across a level surface and collides with a light spring-loaded guardrail. A) neglecting friction, what is the maximum distance the spring is compressed if the spring constant is 1.0 x 106 N/m. B) Calculate the max. acceleration of the car after contact with the spring, again neglect friction. C) if the spring is compressed by only 0.30 m, find the energy lost through friction.

22 Velocity as a Function of Position Conservation of Energy allows a calculation of the velocity of the object at any position in its motion Conservation of Energy allows a calculation of the velocity of the object at any position in its motion Speed is a maximum at x = 0 Speed is a maximum at x = 0 Speed is zero at x = ±A Speed is zero at x = ±A The ± indicates the object can be traveling in either direction The ± indicates the object can be traveling in either direction

23 Sample Problem 13.4 A kg object connected to a light spring with a spring- constant of 20.0 N/m oscillates on a frictionless horizontal surface. A) calculate the total energy of the system and max. Speed of the object if the amplitude of the motion is 3.00 cm. B) what is the velocity of the object when the displacement is 2.00 cm? C) compute the KE and PE of the system when the displacement is 2.00 cm. ( J; m/s; m/s; J; J) A kg object connected to a light spring with a spring- constant of 20.0 N/m oscillates on a frictionless horizontal surface. A) calculate the total energy of the system and max. Speed of the object if the amplitude of the motion is 3.00 cm. B) what is the velocity of the object when the displacement is 2.00 cm? C) compute the KE and PE of the system when the displacement is 2.00 cm. ( J; m/s; m/s; J; J)

24 Simple Harmonic Motion and Uniform Circular Motion 13.3 A ball is attached to the rim of a turntable of radius A A ball is attached to the rim of a turntable of radius A The focus is on the shadow that the ball casts on the screen The focus is on the shadow that the ball casts on the screen When the turntable rotates with a constant angular speed, the shadow moves in simple harmonic motion When the turntable rotates with a constant angular speed, the shadow moves in simple harmonic motion

25 Period and Frequency from Circular Motion Period Period This gives the time required for an object of mass m attached to a spring of constant k to complete one cycle of its motion This gives the time required for an object of mass m attached to a spring of constant k to complete one cycle of its motion Frequency Frequency Units are cycles/second or Hertz, Hz Units are cycles/second or Hertz, Hz

26 Angular Frequency The angular frequency is related to the frequency The angular frequency is related to the frequency

27 Sample problem 13.5 A 1300 kg car is constructed on a frame supported by four springs. Each spring has a spring constant of 20,000 N/m. If two people riding in the car have a combined mass of 160 kg, find the frequency of vibration of the car when it is driven over a pothole in the road. Find also the period and the angular frequency. (1.18 Hz; s; 7.41 rad/s) A 1300 kg car is constructed on a frame supported by four springs. Each spring has a spring constant of 20,000 N/m. If two people riding in the car have a combined mass of 160 kg, find the frequency of vibration of the car when it is driven over a pothole in the road. Find also the period and the angular frequency. (1.18 Hz; s; 7.41 rad/s)

28 Motion as a Function of Time 13.4 Use of a reference circle allows a description of the motion Use of a reference circle allows a description of the motion x = A cos (2πƒt) x = A cos (2πƒt) x is the position at time t x is the position at time t x varies between +A and -A x varies between +A and -A

29 Graphical Representation of Motion When x is a maximum or minimum, velocity is zero When x is a maximum or minimum, velocity is zero When x is zero, the velocity is a maximum When x is zero, the velocity is a maximum When x is a maximum in the positive direction, a is a maximum in the negative direction When x is a maximum in the positive direction, a is a maximum in the negative direction

30 Verification of Sinusoidal Nature This experiment shows the sinusoidal nature of simple harmonic motion This experiment shows the sinusoidal nature of simple harmonic motion The spring mass system oscillates in simple harmonic motion The spring mass system oscillates in simple harmonic motion The attached pen traces out the sinusoidal motion The attached pen traces out the sinusoidal motion

31 Sample problem 13.6 If the object-spring system is described by x=(0.330m)cos (1.50t), find the amplitude, the angular frequency, the frequency, the period, and the position of when t=0.250 s. (0.330m; 1.50 rad/s; Hz; 4.19 s; m) If the object-spring system is described by x=(0.330m)cos (1.50t), find the amplitude, the angular frequency, the frequency, the period, and the position of when t=0.250 s. (0.330m; 1.50 rad/s; Hz; 4.19 s; m)

32 Simple Pendulum 13.5 The simple pendulum is another example of simple harmonic motion The simple pendulum is another example of simple harmonic motion The force is the component of the weight tangent to the path of motion The force is the component of the weight tangent to the path of motion F = - m g sin θ F = - m g sin θ

33 Simple Pendulum, cont In general, the motion of a pendulum is not simple harmonic In general, the motion of a pendulum is not simple harmonic However, for small angles, it becomes simple harmonic However, for small angles, it becomes simple harmonic In general, angles < 15° are small enough In general, angles < 15° are small enough sin θ = θ sin θ = θ F = - m g θ F = - m g θ This force obeys Hookes Law This force obeys Hookes Law

34 Period of Simple Pendulum This shows that the period is independent of of the amplitude This shows that the period is independent of of the amplitude The period depends on the length of the pendulum and the acceleration of gravity at the location of the pendulum The period depends on the length of the pendulum and the acceleration of gravity at the location of the pendulum

35 Sample problem 13.7 Using a small pendulum of length m, a geophysicist counts 72.0 complete swings in a time of 60.0 s. What is the value of g in this location? (9.73 m/s 2 ) Using a small pendulum of length m, a geophysicist counts 72.0 complete swings in a time of 60.0 s. What is the value of g in this location? (9.73 m/s 2 )

36 Simple Pendulum Compared to a Spring-Mass System

37 Damped Oscillations 13.6 Only ideal systems oscillate indefinitely Only ideal systems oscillate indefinitely In real systems, friction retards the motion In real systems, friction retards the motion Friction reduces the total energy of the system and the oscillation is said to be damped Friction reduces the total energy of the system and the oscillation is said to be damped

38 Damped Oscillations, cont. Damped motion varies depending on the fluid used Damped motion varies depending on the fluid used With a low viscosity fluid, the vibrating motion is preserved, but the amplitude of vibration decreases in time and the motion ultimately ceases With a low viscosity fluid, the vibrating motion is preserved, but the amplitude of vibration decreases in time and the motion ultimately ceases This is known as underdamped oscillation This is known as underdamped oscillation

39 More Types of Damping With a higher viscosity, the object returns rapidly to equilibrium after it is released and does not oscillate With a higher viscosity, the object returns rapidly to equilibrium after it is released and does not oscillate The system is said to be critically damped The system is said to be critically damped With an even higher viscosity, the piston returns to equilibrium without passing through the equilibrium position, but the time required is longer With an even higher viscosity, the piston returns to equilibrium without passing through the equilibrium position, but the time required is longer This is said to be over damped This is said to be over damped

40 Damping Graphs Plot a shows a critically damped oscillator Plot a shows a critically damped oscillator Plot b shows an overdamped oscillator Plot b shows an overdamped oscillator

41 Wave Motion 13.7 A wave is the motion of a disturbance A wave is the motion of a disturbance Mechanical waves require Mechanical waves require Some source of disturbance Some source of disturbance A medium that can be disturbed A medium that can be disturbed Some physical connection between or mechanism though which adjacent portions of the medium influence each other Some physical connection between or mechanism though which adjacent portions of the medium influence each other All waves carry energy and momentum All waves carry energy and momentum

42 Types of Waves -- Transverse In a transverse wave, each element that is disturbed moves perpendicularly to the wave motion In a transverse wave, each element that is disturbed moves perpendicularly to the wave motion

43 Types of Waves -- Longitudinal In a longitudinal wave, the elements of the medium undergo displacements parallel to the motion of the wave In a longitudinal wave, the elements of the medium undergo displacements parallel to the motion of the wave A longitudinal wave is also called a compression wave A longitudinal wave is also called a compression wave

44 Waveform – A Picture of a Wave The red curve is a snapshot of the wave at some instant in time The red curve is a snapshot of the wave at some instant in time The blue curve is later in time The blue curve is later in time A is a crest of the wave A is a crest of the wave B is a trough of the wave B is a trough of the wave

45 Longitudinal Wave Represented as a Sine Curve A longitudinal wave can also be represented as a sine curve A longitudinal wave can also be represented as a sine curve Compressions correspond to crests and stretches correspond to troughs Compressions correspond to crests and stretches correspond to troughs

46 Description of a Wave 13.8 Amplitude is the maximum displacement of string above the equilibrium position Amplitude is the maximum displacement of string above the equilibrium position Wavelength, λ, is the distance between two successive points that behave identically Wavelength, λ, is the distance between two successive points that behave identically

47 Speed of a Wave v = ƒ λ v = ƒ λ Is derived from the basic speed equation of distance/time Is derived from the basic speed equation of distance/time This is a general equation that can be applied to many types of waves This is a general equation that can be applied to many types of waves

48 Sample problem 13.8 A wave traveling in the positive x-direction is pictured. Find the amplitude, wavelength, speed and period of the wave if it has a frequency of 8.00 Hz. (0.150 m; m; 3.20 m/s; s) A wave traveling in the positive x-direction is pictured. Find the amplitude, wavelength, speed and period of the wave if it has a frequency of 8.00 Hz. (0.150 m; m; 3.20 m/s; s)

49 Speed of a Wave on a String 13.9 The speed on a wave stretched under some tension, F The speed on a wave stretched under some tension, F The speed depends only upon the properties of the medium through which the disturbance travels The speed depends only upon the properties of the medium through which the disturbance travels

50 Sample problem To what tension must a string with mass kg and length 2.50 m be tightened so that waves will travel on it at a speed of 125 m/s? To what tension must a string with mass kg and length 2.50 m be tightened so that waves will travel on it at a speed of 125 m/s?

51 Interference of Waves Two traveling waves can meet and pass through each other without being destroyed or even altered Two traveling waves can meet and pass through each other without being destroyed or even altered Waves obey the Superposition Principle Waves obey the Superposition Principle If two or more traveling waves are moving through a medium, the resulting wave is found by adding together the displacements of the individual waves point by point If two or more traveling waves are moving through a medium, the resulting wave is found by adding together the displacements of the individual waves point by point Actually only true for waves with small amplitudes Actually only true for waves with small amplitudes

52 Constructive Interference Two waves, a and b, have the same frequency and amplitude Two waves, a and b, have the same frequency and amplitude Are in phase Are in phase The combined wave, c, has the same frequency and a greater amplitude The combined wave, c, has the same frequency and a greater amplitude

53 Constructive Interference in a String Two pulses are traveling in opposite directions Two pulses are traveling in opposite directions The net displacement when they overlap is the sum of the displacements of the pulses The net displacement when they overlap is the sum of the displacements of the pulses Note that the pulses are unchanged after the interference Note that the pulses are unchanged after the interference

54 Destructive Interference Two waves, a and b, have the same amplitude and frequency Two waves, a and b, have the same amplitude and frequency They are 180° out of phase They are 180° out of phase When they combine, the waveforms cancel When they combine, the waveforms cancel

55 Destructive Interference in a String Two pulses are traveling in opposite directions Two pulses are traveling in opposite directions The net displacement when they overlap the displacements of the pulses subtract The net displacement when they overlap the displacements of the pulses subtract Note that the pulses are unchanged after the interference Note that the pulses are unchanged after the interference

56 Reflection of Waves – Fixed End Whenever a traveling wave reaches a boundary, some or all of the wave is reflected Whenever a traveling wave reaches a boundary, some or all of the wave is reflected When it is reflected from a fixed end, the wave is inverted When it is reflected from a fixed end, the wave is inverted

57 Reflected Wave – Free End When a traveling wave reaches a boundary, all or part of it is reflected When a traveling wave reaches a boundary, all or part of it is reflected When reflected from a free end, the pulse is not inverted When reflected from a free end, the pulse is not inverted


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