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UW-Madison PHYSICS 207 - Lecture 27 - Chapter 20

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Lecture 27, Dec. 3WavesEnergy is transported in wave but the motion of matter is localTypes of WavesWave GraphsWave SpeedWave FormsContinuous Sinusoidal WaveWave Properties...Exercise Wave MotionWave PropertiesLook at the temporal (time-dependent) partExercise Wave MotionSlide 14Exercise Wave MotionSound, A special kind of longitudinal waveSoundSpeed of Sound Waves, GeneralWaves on a string...Slide 20Speed of Sound in a Solid RodWaves, Wave fronts, and RaysSlide 23Waves, Wavefronts, and RaysExercise Spherical WavesIntensity of soundsSlide 27Sound Level, ExampleLoudness and IntensityDoppler effect, moving sources/receiversDoppler effect, moving sources/receiversSlide 32Physics 207: Lecture 27, Pg 1Lecture 27, Dec. 3Goals:Goals:•Chapter 20Chapter 20 Employ the wave model Visualize wave motion Analyze functions of two variables Know the properties of sinusoidal waves, including wavelength, wave number, phase, and frequency. Work with a few important characteristics of sound waves. (e.g., Doppler effect)•AssignmentAssignment HW11, Due Friday, Dec. 5th  HW12, Due Friday, Dec. 12th  For Monday, Read through all of Chapter 21Physics 207: Lecture 27, Pg 2WavesA traveling wave is an organized disturbance propagating at a well-defined wave speed v.In transverse waves the particles of the medium move perpendicular to the direction of wave propagation.In longitudinal waves the particles of the medium move parallel to the direction of wave propagation.A wave transfers energy, but no material or substance is transferred outward from the source.Physics 207: Lecture 27, Pg 3Energy is transported in wave but the motion of matter is localPhysics 207: Lecture 27, Pg 4Types of WavesMechanical waves travel through a material medium such as water or air.Electromagnetic waves require no material medium and can travel through vacuum.Matter waves describe the wave-like characteristics of atomic-level particles.For mechanical waves, the speed of the wave is a property of the medium. Speed does not depend on the size or shape of the wave.Examples: Sound waves (air moves locally back & forth) Stadium waves (people move up & down) Water waves (water moves up & down) Light waves (an oscillating electromagnetic field)Physics 207: Lecture 27, Pg 5Wave GraphsThe displacement D of a wave is a function of both position (where) and time (when).A snapshot graph shows the wave’s displacement as a function of position at a single instant of time.A history graph shows the wave’s displacement as a function of time at a single point in space.The displacement, D, is a function of two variables, x and t, or D(x,t)Physics 207: Lecture 27, Pg 6Wave SpeedSpeed of a transverse, mechanical wave on a string: where Ts is the string tension and  is linear string densitySpeed of sound (longitudinal mechanical wave) in air at 20°Cv = 343 m / sSpeed of light (transverse, EM wave) in vacuum: c = 3x108 m/sSpeed of light (transverse, EM wave) in a medium: v = c / nwhere n = index of refraction of the medium (typically 1 to 4)property inertialproperty elasticv sTvLmPhysics 207: Lecture 27, Pg 7Wave FormsSo far we have examined “continuous wavescontinuous waves” that go on forever in each direction !v v We can also have “pulses” caused by a brief disturbanceof the medium:v And “pulse trains” which aresomewhere in between.Physics 207: Lecture 27, Pg 8Continuous Sinusoidal WaveWavelengthWavelength: The distance  between identical points on the wave.Amplitude: The maximum displacement A of a point on the wave.AAnimationPhysics 207: Lecture 27, Pg 9Wave Properties...Period: The time T for a point on the wave to undergo one complete oscillation.Speed: The wave moves one wavelength  in one period T so its speed is v = / T.TvAnimationPhysics 207: Lecture 27, Pg 10Exercise Wave MotionThe speed of sound in air is a bit over 300 m/s, and the speed of light in air is about 300,000,000 m/s. Suppose we make a sound wave and a light wave that both have a wavelength of 3 meters. What is the ratio of the frequency of the light wave to that of the sound wave ? (Recall v = / T = f )(A) About 1,000,000(B) About 0.000,001(C) About 1000Physics 207: Lecture 27, Pg 11Wave PropertiesLook at the spatial part (Let t =0).Animation])//(2cos[(),(0 TtxAtxD)] )/2cos[()0,( xAxDWavelengthAyx•x = 0 y = A•x = /4 y = A cos(/2) = 0•x = /2 y = A cos() = -A]cos[),(0 tkxAtxDA = amplitude k = 2/ = wave number= 2f = angular frequency 0= phase constantPhysics 207: Lecture 27, Pg 12Look at the temporal (time-dependent) partLet x = 0)] )/2cos[(),( txAtxDPeriodAyt] )/2(cos[)cos(),0( tTAtAtD•t = 0 y = A•t =T / 4 y = A cos(-/2) = 0•t =T / 2 y = A cos(-) = -APhysics 207: Lecture 27, Pg 13Exercise Wave MotionA harmonic wave moving in the positive x direction can be described by the equation (The wave varies in space and time.) v =  / T =  f = (   ) ( f) =  / k and, by definition,  > 0D(x,t) = A cos ( (2 /) x - t ) = A cos (k x – t )Which of the following equation describes a harmonic wave moving in the negative x direction ?(A) D(x,t) = A sin (k x  t )(B) D(x,t) = A cos ( k x  t )(C) D(x,t) = A cos ( k x  t )Physics 207: Lecture 27, Pg 14Exercise Wave MotionA boat is moored in a fixed location, and waves make it move up and down. If the spacing between wave crests is 20 meters and the speed of the waves is 5 m/s, how long t does it take the boat to go from the top of a crest to the bottom of a trough ? (Recall v = / T = f )(A) 2 sec (B) 4 sec (C) 8 sectt + tPhysics 207: Lecture 27, Pg 15Exercise Wave MotionA boat is moored in a fixed location, and waves make it move up and down. If the spacing between wave crests is 20 meters and the speed of the waves is 5 m/s, how long t does it take the boat to go from the top of a crest to the bottom of a trough ? T = 4 sec but crest to trough is half a wavelength(A) 2 sec (B) 4 sec (C) 8 sectt + tPhysics 207: Lecture 27, Pg 16Sound, A special kind of longitudinal waveConsider a vibrating guitar stringString VibratesPiece of string undergoes harmonic motionAir molecules


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UW-Madison PHYSICS 207 - Lecture 27 - Chapter 20

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