QUICK QUIZ 16.1 (end of section 16.2)

Slides:



Advertisements
Similar presentations
In Example 18.1, we discovered that a listener at point P would hear a minimum in the sound when the oscillator driving both speakers was at a frequency.
Advertisements

Chapter 16 Wave Motion.
QUICK QUIZ 15.1 (end of section 15.2)
Physics for Scientists and Engineers, 6e
Section 3.2 and 3.3.
Chapter 20.
Determining Wave Speed
Waves Tanya Liu. What is a wave? A wave is a disturbance or oscillation that is a function of space and time, involves a transfer of energy Surface wave.
Chapter 13 Mechanical waves. Traveling waves If we perturb again and again we create a series of pulses One can do the same with a spring or a rope When.
Simple Harmonic Motion
Spring 2002 Lecture #23 Dr. Jaehoon Yu 1.Superposition and Interference 2.Speed of Waves on Strings 3.Reflection and Transmission 4.Sinusoidal.
Vibrations and Waves. AMPLITUDE WAVELENGTH CREST TROUGH.
Experiment with the Slinky
Chapter 16 Wave Motion.
Some Oscillating Systems Object on a vertical spring Choose downward direction as positive Spring force on mass is -ky where y is downward displacement.
بسم الله الرحمن الرحيم.
Chapter Eleven Wave Motion. Light can be considered wavelike by experimental analogies to the behavior of water waves. Experiments with fundamental particles,
Standing Waves Physics 202 Professor Lee Carkner Lecture 7.
Standing Waves Physics 202 Professor Lee Carkner Lecture 8.
1 Fall 2004 Physics 3 Tu-Th Section Claudio Campagnari Web page:
Physics 101: Lecture 32, Pg 1 Physics 101: Lecture 32 Waves and Sound l Today’s lecture will cover Textbook Sections l Review: Simple Harmonic.
16.1 Propagation of a Disturbance
Chapter 16 Waves (I) What determines the tones of strings on a guitar?
Copyright © 2009 Pearson Education, Inc. Lecture 1 – Waves & Sound a) Simple Harmonic Motion (SHM)
Physics 121 Newtonian Mechanics Instructor Karine Chesnel April, 7, 2009.
Chapter 18 Superposition and Standing Waves. Waves vs. Particles Waves are very different from particles. Particles have zero size.Waves have a characteristic.
Objectives Identify the conditions of simple harmonic motion.
NAZARIN B. NORDIN What you will learn: Load transfer, linear retardation/ acceleration Radius of gyration Moment of inertia Simple.
1© Manhattan Press (H.K.) Ltd. Pulse Continuous waves Continuous waves 8.1 Characteristics of waves Wave motion Wave motion Graphical representation of.
FCI. Faculty of Computers and Information Fayoum University 2014/ FCI.
Waves Chapter 16:Traveling waves Chapter 18:Standing waves, interference Chapter 37 & 38:Interference and diffraction of electromagnetic waves.
Chapter 11 - Simple Harmonic Motion
Section 1 Simple Harmonic Motion
Wave motion and its equations Harmonic waves Waves on a string
Chapter 11 Vibrations and Waves Phy 2053 Conceptual Questions.
Chapter 11 Preview Objectives Hooke’s Law Sample Problem
Oscillations (continues) Vibrating systems What we studied before? Simple harmonic motion (one mode) Mass on spring Simple pendulum (SHM for small angles)
CP Physics Chapter 12 Waves. Hooke’s Law F spring = kx During the periodic motion At equilibrium, velocity reaches a maximum (b) At maximum displacement,
1 Waves and Vibrations. 2 Types of Waves Mechanical waves water, sound & seismic waves *governed by Newton’s laws *only exist within material medium Electromagnetic.
Phys211C19-20 p1 Waves A pulse on a string (demos) speed of pulse = wave speed = v depends upon tension T and inertia (mass per length  ) y = f(x  vt)
Simple Harmonic Motion. Restoring Forces in Spring  F=-kx  This implies that when a spring is compressed or elongated, there is a force that tries to.
1 Vibrations & Waves Test Review Find a friend and a whiteboard for this activity!
Vibrations and Waves Chapter 12. Simple Harmonic Motion A motion that occurs repeatedly, vibrating back and forth over its equilibrium point. The force.
Chapter 16: Waves and Sound  We now leave our studies of mechanics and take up the second major topic of the course – wave motion (though it is similar.
Q13. Oscillatory Motion Q14. Wave Motion
Chapter 16 Waves-I Types of Waves 1.Mechanical waves. These waves have two central features: They are governed by Newton’s laws, and they can exist.
Chapter 16 Waves-I Types of Waves 1.Mechanical waves. These waves have two central features: They are governed by Newton’s laws, and they can exist.
Chapter 14: Waves and Sound  We now leave our studies of mechanics and take up the second major topic of the course – wave motion (though it is similar.
Wednesday, Dec. 3, 2003PHYS , Fall 2003 Dr. Jaehoon Yu 1 PHYS 1443 – Section 003 Lecture #24 Wednesday, Dec. 3, 2003 Dr. Jaehoon Yu 1.Sinusoidal.
Vibrations & Waves Chapter 11. Simple Harmonic Motion Periodic motion = repeated motion Good example of periodic motion is mass on a spring on a frictionless.
Copyright © 2010 Pearson Education, Inc. Chapter 13 Oscillations about Equilibrium.
6  When waves are combined in systems with boundary conditions, only certain allowed frequencies can exist. › We say the frequencies are quantized.
Waves and Energy Transfer Surf’s Up Braaaaaaaaaaaaah.
Reference Book is. Introduction mechanical waves electromagnetic wavesMechanical waves Waves are two main types : mechanical waves and electromagnetic.
Q14.Wave Motion. 1.The displacement of a string carrying a traveling sinusoidal wave is given by 1. v 0 /  y 0 2.  y 0 / v 0 3.  v 0 / y 0 4. y.
Quiz “2” for Waves For First Year 2015/2016 Faculty of Computers and Information Fayoum University FCI.
Section 1 Simple Harmonic Motion
9. Two-mass vibrator Longitudinal vibration
9. Two-mass vibrator Longitudinal vibrations
Oscillations (continues)
Waves A pulse on a string (demos) speed of pulse = wave speed = v
Waves Chapter 16: Traveling waves
Intro Question 1 A wave pulse is created by very sharply moving the free-end of a cord (or spring) to the side and back to its original position. How.
Constant Force (F = constant)
بسم الله الرحمن الرحيم FCI.
Traveling Waves Waves and Sound
Mechanical Waves A mechanical wave is a physical disturbance in an elastic medium. Consider a stone dropped into a lake. Energy is transferred from stone.
Oscillations (continues)
CHAPTER-16 T071,T062, T061.
Physics 20 Mechanical Waves
Presentation transcript:

QUICK QUIZ 16.1 (end of section 16.2) While sitting at the beach, you count the number of waves that hit the beach during a certain amount of time. This measurement is most closely associated with a) the period of the waves, b) the frequency of the waves, c) the wavelength of the waves, or d) the speed of the waves.

QUICK QUIZ 16.1 ANSWER (b). The frequency of a wave is associated with the number of cycles of the wave that occur in a given amount of time. When we count the waves that hit the beach, we are actually counting the number of wave crests.

QUICK QUIZ 16.2 (end of section 16.2) In Equation 16.10, y = A sin(kx – wt), for a traveling sinusoidal wave, the variable, k, is related to the spring constant, k, from Chapter 15 a) in the sense that it is related to a force, b) in the sense that it is associated with a displacement, c) in the sense that it is associated with oscillatory motion, or d) is not related to the spring constant, k.

QUICK QUIZ 16.2 ANSWER (d). Unfortunately, when representing the large quantity of physical variables that exist, the alphabet becomes quickly exhausted. The variable k is used for two completely different quantities, the spring constant and the wave number. These quantities must be completely different since the units are completely different.

QUICK QUIZ 16.3 (end of section 16.3) You suspend an object from the end of a hanging rubber band, send a pulse along the band and measure the speed of the pulse to be v. You then quadruple the mass of the object that you hang on the rubber band and the rubber band’s length increases by a factor of two from its original length with the first object. If you now send a pulse along the band, the speed of the pulse will be a) v/(22) b) v/2, c) v/2, d) v, e) 2 v, f) 2v, or g) (22)v

QUICK QUIZ 16.3 ANSWER (g). By increasing the mass of the hanging object by a factor of four, you have increased the tension by a factor of four. Since the rubber band has doubled its length, its mass per unit length or linear mass density has gone down by a factor of two. Therefore,

QUICK QUIZ 16.4 (end of section 16.5) You perform an experiment on a string and generate sinusoidal waves of an amplitude, A, and frequency, f. You then perform a similar experiment on a string that has twice the linear mass density and which is under half the tension as the original string. To generate sinusoidal waves of an amplitude, A, and frequency, f, in this new string, you will have to transfer energy to the new string at a rate that is a) one fourth the rate for the original string, b) half the rate for the original string, c) the same as the rate for the original string, d) twice the rate for the original string, or e) four times the rate for the original string.

QUICK QUIZ 16.4 ANSWER (c). Equation 16.21 relates the energy rate transfer to the linear mass density, frequency, amplitude and speed. The speed is in turn related to the tension and the linear mass density so that the equation may be rewritten, Therefore, if one doubles the linear mass density and halves the tension, the rate of energy transfer must remain the same to keep the same amplitude and frequency.

QUICK QUIZ 16.5 (end of section 16.6) Which of the following is a solution to the linear wave equation? a) y = x + vt2, b) y = sin2(x + vt), c) both a and b, d) neither a nor b.

QUICK QUIZ 16.5 ANSWER (b). Only functions of the form y = f(x ± vt) are solutions to the wave equation. The function y = x + vt2 is not of this form and it is easy to verify that it is not a solution. We have, Since 0 is not, in general, equal to 2/v, the function is not a solution to the wave equation. On the other hand, y = sin2(x + vt) is of the form y = f (x ± vt) and is a solution to the wave equation. We have,