XI PHYSICS [WAVES AND SOUND] CHAPTER NO. 8. M. Affan Khan LECTURER PHYSICS, AKHSS, K.

Transcription

1 XI PHYSICS M. Affan Khan LECTURER PHYSICS, AKHSS, K affan_414@live.com [WAVES AND SOUND] CHAPTER NO. 8

2 OSCILLATORY MOTION A motion in which an object moves to and fro or up and down about a fixed point is called oscillatory or vibratory motion. SIMPLE HARMONIC MOTION (S.H.M) An oscillatory motion in which acceleration is directly proportional to the displacement and is always directed toward the mean position is called simple harmonic motion. Mathematically, a x Here negative shows that acceleration is always directed towards its mean position. CONDITIONS For simple harmonic motion following conditions must be satisfied. The system must have property of inertia. A restoring force is required. Motion must be oscillatory. Acceleration must be directly proportional to the displacement. CHARACTERISTICS A simple harmonic motion has following characteristics. Oscillatory motion. Time period Frequency Amplitude MOTION OF MASS SPRING SYSTEM Consider an object of mass m placed on a horizontal frictionless surface. Let this mass is attached with a spring of spring constant k as shown in figure. If an external force is applied to the object and it covers some displacement x than the restoring force can be found by using Hook s law, F = - k x (1) Where negative shows that restoring force is opposite to the applied force. According to the Newton s nd law F = m a () Comparing equation (1) and ()

3 ma = kx a = k m x This is the equation of acceleration of mass spring system Since k/m is constant, therefore a x Result: This expression shows that motion of mass spring system is simple harmonic. TIME PERIOD: Acceleration of mass spring system is given by, a = x k m Since mass spring system is a simple harmonic oscillator therefore its acceleration can also be written as, a = ω x Comparing above two accelerations we have, ω x = x k m ω = k m But also, ω = π T π T = k m T = π m k The above relation shows that time period of mass spring system is directly proportional to the square root of mass and inversely proportional to the square root of spring constant. FREQUENCY: Number of vibration or oscillation or rotation per second is called frequency. OR The reciprocal of time period is called frequency UNIT: S.I unit of frequency is per second or hertz.

4 FREQUENCY OF MASS SPRING SYSTEM: As we know that time period of spring mass system is, T = π m k But, f = 1 T Therefore, f = 1 π k m It is clear from this formula that time period of simple pendulum is independent of mass of the bob and it depends upon length of the string. RELATION BETWEEN UNIFORM CIRCULAR MOTION AND SIMPLE HARMONIC MOTION: Let us consider a particle of mass m moving around a vertical circle of radius x 0 with constant angular velocity ω. If θ is the angular displacement swept during time t then θ = ωt. The projection θ of particle P on the diameter AB of the circle as P moves along circular path. It is also observed that the projection Q speeds up when it moves towards the center O and slows down when it moves away from the center. Thus the instantaneous acceleration of projection Q is directed towards the center and it has vibratory motion. Now, to show that motion of Q is simple harmonic, we calculate its acceleration. The motion of Q is associated with the motion of P hence the acceleration of Q must be a component of the acceleration of the motion of particle P. The acceleration of the particle P is centripetal acceleration i.e. directed towards the centre of the circle along the line PO and it given by, a c = v r

5 Or a c = v p x 0 a c = x 0ω x 0 a c = x 0 ω The acceleration of projection Q is equal to the component of acceleration of particle P along x-axis i.e. In right triangle POQ. a x = a c cosθ (1) cosθ = OQ OP cosθ = x x 0 Putting the values of centripetal acceleration and cosθ, we get, a x = x 0ω x x 0 a x = ω x a x x Hence it is proved that the motion of projection Q is simple harmonic. i) Instantaneous Displacement At some instant of time t, the angle between OP and the x-axis is θ. In right angled triangle POQ cosθ = OQ OP cosθ = x x 0 x = x 0 cosθ If θ = ωt + ϕ, where ϕ is the initial phase angle at time t = 0. So we may write x = x 0 cos (ωt + ϕ) This expression represents instantaneous displacement of projection Q and its value lies between +x 0 and x 0. Where x 0 is called amplitude of SHM of projection Q. ii) Instantaneous Velocity As the motion of Q depends upon the motion of P then the speed of projection Q is equal to the horizontal component of the speed of the particle P, i.e.

6 From trigonometry, sinθ = RP PS sinθ = V x V p V x = V p sinθ V x = x 0 ωsinθ cos θ + sin θ = 1 sinθ = 1 cos θ sinθ = 1 ( x ) x 0 sinθ = x 0 x x 0 Now, we can substitute value of sine in above equation, V x = x 0 ω x 0 x x 0 V x = ω x 0 x As x is instantaneous displacement then V x will be instantaneous velocity of projection Q, i.e. at any time t. ENERGY OF A PARTICLE EXECUTING SHM Let us consider a body of mass m connected with one end of a spring whose other end is connected with rigid wall and it can execute SHM on a frictionless surface as shown in fig. Now we find expression for instantaneous kinetic and potential energies: i) Kinetic Energy When displacement of body from its mean position is x then instantaneous velocity will be, V = ω x 0 x Where x0 is the amplitude of SHM We have ω = k m

7 V = k m x 0 x As we know that K. E = 1 mv K. E = 1 m [ k m x 0 x ] When x = ±x 0 Then K. E = 1 (x 0 x 0 ) K. E = 0 i.e minimum K. E = 1 m k m (x 0 x ) K. E = 1 k(x 0 x ) When x = 0 Then K. E = 1 kx 0 i.e maximum ii) Potential Energy According to Hooke s law, the magnitude of restoring force acting on a body attached with spring at displacement x from its mean position is F = kx At mean position, F = 0 Therefore the average force on the mass m during displacement x is F = 0 + kx = 1 kx Now, W = F. x W = Fxcosθ W = ( 1 kx) xcos00 Here W = P. E Therefore, W = 1 kx P. E = 1 kx Total Energy At any instant of SHM the body has partly P.E. and partly K.E. Therefore, total energy at any instant will be

8 E = P. E + K. E E = 1 kx + 1 k(x 0 x ) E = 1 kx + 1 kx 0 1 kx E = 1 kx 0 Here amplitude factor defines the maximization which clearly states that the total energy at every point is constant and there will be just a conversion of K.E to P.E or P.E to K.E. SIMPLE PENDULUM A system which consist of a point mass (spherical bob) suspended by a light, flexible and inextensible string tied to a fixed rigid and frictionless support is called simple pendulum. When the bob is displaced from its mean position and then released, it begins to oscillate periodically which is one of the condition of SHM. To check whether its motion is simple harmonic or not, we find acceleration of the motion of the bob. Let us consider a bob of a mass m and weight W is suspended by means of inextensible light string of length l. If the amplitude of oscillation is very small, then its motion will be SHM. When the displacement of bob is x from its mean position, then its weight W can be resolved into its components as shown in fig. cosθ = W W => W = Wcosθ sinθ = W W => W = Wsinθ The components of weight W along the length of string is just balanced by the tension in the string i.e. T = W T = Wcosθ Hence the net force acting on the bob is W, which is responsible for the oscillation of the bob i.e. F = W F = Wsinθ Here ve sign indicates that the force is directed towards mean position. According to Newton s second law of motion, F = ma Therefore,

9 ma = mgsinθ a = gθ As we know that S = rθ Here, We may write now, x = lθ => θ = x l As the string is inextensible then g l = constant a = g( x l ) a = (constant)x a x This result shows that the motion of simple pendulum is simple harmonic. TIME PERIOD As we know that the acceleration of SHM of projection of circular motion of a particle is, a = ω x By comparing of acceleration for Simple Pendulum with the above equation, we get As we know that ω = ( g l ) => ω = ( g l ) 1 By putting the value of ω we get T = π ω T = π l g

10 WAVE MOTION The mechanism by which energy is transferred from one place to another is called wave motion. Types of Waves We can categorize the types of waves in 3 categories. a) W.r.t medium b) W.r.t propagation c) W.r.t mode of vibration a) Types of Waves w.r.t Medium i) Mechanical Waves ii) Electromagnetic Waves Mechanical waves are those which require a medium for their propagation, whereas, electromagnetic waves are those which do not require any medium for their propagation. For example sound waves are mechanical and light waves are electromagnetic in nature. b) Types of Waves w.r.t mode of vibration i) Longitudinal Waves ii) Transverse Waves i) Longitudinal Waves Such waves in which particles of the disturbed medium undergo displacement in a direction parallel to the direction of wave motion are called longitudinal waves. In the presence of longitudinal waves in a medium, the particles of the medium vibrate parallel to the direction of propagation i.e. these particles move back and forth about their mean position. These waves are produced in substances which are elastic and compressible like gases and wire spring. Also sound waves are longitudinal waves as disturbance corresponds to a series of high and low pressure regions that travel through air or through any other material medium with certain velocity. Similarly a longitudinal pulse can be produced in a spring as shown in fig. ii) Transverse Waves Such waves in which particles of the medium vibrate in a direction perpendicular to the propagation of waves are called transverse

11 waves. E.g. the fig. shows that the wave pulse travels along the rope, each segment of the rope which is disturbed moves in a direction perpendicular to the wave motion and there is no motion in any part of rope in the direction of propagation of wave. Hence this pulse is transverse wave. Electromagnetic waves such as light x rays, radio and television transmission waves are also transverse. c) Types of waves w.r.t propagation i) Travelling waves ii) Standing waves i) Travelling Waves A travelling wave is that in which the displacement of wave depends upon both time and space. In case of travelling wave through a medium, every particles or segment of the medium vibrate simple harmonically with a frequency equal to the frequency of vibration of the source that drives the wave into the medium. A travelling wave can be produced in a string (medium) by flipping it at on end as shown in fig. above for transverse waves. The shape of the disturbed part of the string containing the wave pulse can be described at a given time mathematically by a wave function f(x) such that y = f(x) Here y is the vertical displacement of a particle from its equilibrium position and x is the horizontal displacement of the particle from the point where the displacement y is zero. Hence x, y, are the coordinates of the position of particles. Since the wave pulse is moving along the string, its position is changing continuously with time. Hence the location of wave pulse depends on time also. Thus the shape of the wave pulse with its location can be given by the function f(x,t) such that y = f(x, t) This is called wave function. For a travelling wave, moving along +x-axis, the wave function will be, y = f(x ) = f(x vt) Sound waves are travelling waves. Similarly, the light waves are also travelling wave. ii) Standing waves The waves formed by superposition or overlapping of two travelling waves of same amplitude and frequency moving in opposite direction in the same medium are called standing waves or stationary waves. When a string is tightly stretched between two fixed supports and then flicked upward, the crest extends over the whole distance between the

12 supports. So each end of the wave suffers a phase change i.e. crest on reflection becomes a trough and the trough becomes a crest on reflection at the other end as shown in fig. These waves are stationary or standing in the sense that these are found in the form of loops in which vibration occur within limited space. The point where displacement is maximum called antinode denoted by A, and that where displacement is minimum (zero) is called a node denoted by N. The distance between two consecutive nodes or any two consecutive antinodes is equal half of the wavelength. SUPERPOSITION PRINCIPLE Whenever two or more waves travel in the same space then these waves interfere with each other, thus form a resultant wave. The net wave displacement caused by resultant wave is found equal to the algebraic sum of the individual wave displacements of all given waves. This is known as superposition principle and it may be written as, Y = y 1 + y + y y n Let us consider two sinusoidal waves with the same amplitude, frequency and wavelength travelling in opposite direction i.e. y 1 = A 0 sin (kx ωt) and y = A 0 sin (kx + ωt) Where, A 0 = Amplitude of wave k = π λ i. e. angular wave number ω = πν = π i. e. angular frequency T x = space or position coordinate t = time coordinate According to superposition principle the resultant wave displacement will be,

13 y = y 1 + y By putting the values, y = A 0 sin (kx ωt) + A 0 sin (kx + ωt) y = A 0 [sin(kx ωt) + sin(kx + ωt)] kx ωt + kx + ωt kx ωt kx + ωt y = A 0 [sin ( ) cos ( )] y = A 0 sinkxcosωt This equation represents the wave function of standing waves having angular frequency ω and resultant amplitude equal to A 0 sinkx. It means that the amplitude of SHM of a given particle of medium or string depends on sinkx in case of standing waves. Points of Maximum Amplitudes or Intensity The resultant amplitude of standing wave is Aosinkx. Therefore, amplitude will be maximum only when, sinkx = ±1 kx = sin 1 (±1) π λ = 900, 70 0, , π λ x = π, 3π, 5π, 7π, x = λ π (π, 3π, 5π, 7π ) x = λ 4, 3λ 4, 5λ 4, 7λ 4, These are the points of maximum amplitudes in standing waves and these are known as Antinodes. The distance between two consecutive antinodes is equal to λ i.e. or 3λ 4 λ 4 = λ 5λ 4 3λ 4 = λ Points of minimum amplitudes or intensity The resultant amplitude of standing wave is, A 0 sinkx Therefore, amplitude will be minimum only when, sinkx = 0 kx = sin 1 0 kx = 0 0, 180 0, 360 0, 540 0, π x = 0, π, π, 3π, 4π λ x = λ (0, π, π, 3π, 4π ) π

14 x = 0, λ 3λ 5λ, λ,, λ, These are the points of minimum amplitudes in standing waves, and these are known as Nodes. The distance between any two consecutive nodes is equal to λ i.e or λ 0 = λ λ λ = λ FUNDAMENTAL FREQUENCY AND HARMONICS Standing waves can be set up by a continuous super position of waves incident and reflected from the extreme points of the medium. Let us consider a stretched string of length L which can vibrate in different modes and each mode has its own frequency as shown in fig. 1 st Harmonics or Fundamental Frequency: If the string is plucked from its midpoint and released it begins to vibrate in one loop by forming nodes at fixed points as shown in fig. As we can see from the diagram the distance between two consecutive nodes is equal to half of the wavelength. Then L = λ 1 Or, λ 1 = L We Have V = νλ In this case we may write with the following subscripts ν 1 = V λ 1 ν 1 = V L This is fundamental frequency, or the 1 st harmonics of standing waves. nd Harmonics or 1 st Overtone If the same string is now vibrated with more frequency then there is a chance that the string must vibrate in two segments.

15 Here the length of string is equal to one complete wavelength L = λ, We Have V = νλ In this case we may write with the following subscripts ν = V λ We may write the above equation as This is called nd harmonics or 1 st overtone. 3 rd Harmonics or nd Overtone ν = V L ν = V L = ( V L ) ν = ν 1 The same string can also vibrate into three segments if it is plucked with more frequency and in this case the length of string forms one and half wavelength L = 3 λ 3, Or λ 3 = L 3 We Have V = νλ In this case we may write with the following subscripts ν 3 = V λ 3 ν 3 = V L/3 ν 3 = 3V L = 3 ( V L ) ν 3 = 3ν 1 This is called 3 rd harmonics or nd overtone By examining the equations of all harmonics we can say that if string vibrates in n loops then, ν n = nν 1

16 SONOMETER: It is a device used to study the vibration of stretched string in different number of loops. It consists of a thin metallic wire stretched across two bridges on the top of a hollow wooden sounding box one meter in length. One end of the wire is fastened to a peg at one end of the box and other end passes over a smooth frictionless pulley is connected with suspended load. By adjusting the position of bridges or by changing the postion of movable bridge C, different modes of vibration can be achieved. If L is the length of vibrating segment of the string, T is the tension and μ is the mass per unit length of the wire, then the frequency produced in the string given by, ν n = nν 1 v n = nv L v n = n L T μ Where n is an integer (indicating mode of vibration) For n = 1 As we can see here clearly in above equation v 1 = 1 L T μ v 1 (Law of Length) L v T (Law of Tension) v 1 (Law of linear density) μ

17 SOUND WAVES Sound is the form of energy and it travels in the form of longitudinal waves. As sound waves are mechanical waves i.e. they travel through a medium then particles of the medium vibrate along the direction of propagation of the wave motion. Sound waves can travel through gases, solids and liquids with a speed which depends upon the properties of the medium. Because of longitudinal displacement of molecules of medium about their mean position, a series of alternate high and low pressure regions called compressions and rarefactions respectively is formed. This series ultimately reaches at ear drum which begins to vibrate with same frequency as the sound waves have. There are three classes of sound waves depending upon frequency, i) Infrasonic waves ii) Audible waves iii) Ultrasonic waves Such longitudinal mechanical waves which have frequency less than 0 Hz are called infrasonic waves Such longitudinal mechanical waves which have frequency range between 0 Hz to 0 khz are called audible sound waves. Such longitudinal mechanical waves which have frequency greater than 0 khz are called ultrasonic waves. SPEED OF SOUND WAVES Newton s Formula The speed of sound in air was determined by Newton through his formula for speed of longitudinal or compressional waves in a medium. As sound waves are also longitudinal or compression waves through a medium then the speed of sound depends upon the compressibility and the inertia of the medium. In fact the high speed of all mechanical waves can be expressed in a general form.

18 (elastic property) V = inertial property Newton developed a formula for speed of sound in waves in air as, V = B ρ Where B is bulk modulus of compressible medium i.e. air and ρ is the density which is inertial property. Bulk modulus is defined as the ratio of stress to the volumetric strain, stress B = volumetric strain B = P V/V Newton assumed that the process of sound propagation is isothermal i.e. in this process temperature remains constant. And in the case of isothermal process bulk modulus is only equal to pressure. B = P Therefore, V = P ρ As we go through this formula, and put values of atmospheric pressure and density at STP, we find that velocity of sound comes out to be 81 m/s, which is completely contradicting with the experimental value of 33 m/s. Therefore, this idea of Newton was rejected. Laplace s Correction Laplace realized that, the wave motion in case of sound is so rapid and the heat conductivity is so low that there is in sufficient time for the heat produced in the compressed regions to be conducted to the rarefied regions, therefore, the process of propagation of sound waves is not isothermal rather it is adiabatic which is a process in which heat does not flow into or out of the system. Laplace, therefore, used adiabatic equation in deriving formula for speed of sound in air as he forced that temperature of medium doesn t remain constant. The modified formula for the speed of sound in air is,

19 V = γp ρ Where, γ is the ratio of molar specific heat of gas at constant pressure to the molar specific heat at constant volume. Effects of Temperature on Speed of Sound i. e. γ = C p C v The speed of sound in any medium increase with the rise in temperature. As the translational and vibrational kinetic energy of molecules of the medium is increased with the rise in temperature then pressure zones propagate more rapidly in the form of alternate compressions and rarefactions after the temperature of medium air is increased. We have the formula for speed of sound in air as, According to general gas equation, P = nrt P = nrt V Putting in above equation V = γp ρ V = γnrt ρ For one mole of gas (i.e. n = 1) V = γnrt M V = γnrt M V = γrt M Also, if we need to find velocity of sound a particular temperature (VT), we may simple use the following formula

20 Where, T K is the temperature in Kelvin. Characteristics of Musical Sound V T = 33 T K 73 Following are the characteristics of Musical Sound i) Loudness ii) Intensity Level iii) Pitch iv) Quality i) Loudness The auditory sensation produced by intensity of sound I called louness of sound. Therefore, it depends upon both intensity of sound and the nature of humar ear. A normal human ear is very sensitive detector sound. It can record the least sound (10-1 Watt/m ) ii) Intensity Level Weber-Fechner s Law The loudness of sound doesn t increase directly as the power delivered to the ear increases but seems to vary roughly as the logarithm of the power or intensity. This was first realized by Weber-Fechner and they stated that, Loudness of sound is directly proportional to the logarithm of intensity L log I L = klogi If I 0 the intensity of faintest audible sound then its loudness can be written as, L 0 = klogi 0 The difference of loudness of sound with the loudness of faintest audible sound is called intensity level. By subtracting L0 from L, we get L L 0 = klogi klogi 0 L L 0 = k(logi logi 0 ) L L 0 = klog ( I I 0 )

21 Where L L 0 = β (intensity level) β = klog ( I ) I 0 Unit In M.K.S system the unit of intensity level is Bel. As it is a large unit so we measure intensity level in decibel (db) i.e. 1 Bel = 10 db The unit of loudness of sound is Sone. 1 Sone = 40dB at 1000 Hz. iii) Pitch The pitch of sound reflects its class of frequency. It is the property of sound by which we can distinguish between shrill and grave sound. The greater the frequency, the greater will be the pitch of sound and lower the frequency, the lower will be the pitch of sound. For example, the frequency of women s sound is more than the men s sound. Therefore, the women s sound will be considered as shrill and the men s sound will be considered as grave normally. iv) Quality of Sound (or Timbre) The quality of sound is the property by which we can distinguish between nodes of the same pitch and intensity when played on different instruments or sung by different voices. Every instruments of the same kind may yield notes of different quality. We recognize the voice of our friend over the telephone by its quality. The difference in the sound produced by two notes of same pitch and loudness is due to difference in their resultant waveforms. The resultant waveform of any sound is obtained by combining the amplitudes of fundamental and the overtones of given sound. Difference between Musical Sound and Noise The difference between noise and musical sound is because of the waveform of sound. If the wave form is irrefular non-symmeteric and having random fluctuations then resulting sound is said to be noise. Similarly, if the wave form is regular and symmetrical and having ordered fluctuations then resulting sound produces a smooth pleasant sensation, hence called music.

22 BEATS The periodic vibration in the intensity of sound at a given point due to superposition of two waves having slightly different frequencies is called the phenomenon of beats. The production of beats is actually the interference of sound waves having slightly different frequencies due to which intensity of resultant wave changes in time constructively and destructively. The number of beats that one hear per second (beat frequency) is equal to the difference in frequency between two sources. The maximum beat frequency that the human ear can detect is about 7 beats per second. When the beat frequency (number of beats produced per second) is greater than seven we cannot hear them clearly. If we strike two tuning forks of slightly different frequencies with a rubber pad and bring them in air then we hear only one note of changing intensity i.e. periodic rise and fall in the intensity of sound. This is called phenomenon of beats. Consider two travelling waves having equal amplitudes but slightly different frequencies f1 and f in the same direction i.e. Y 1 = A 0 cosω 1 t; Y = A 0 cosω t Y = Y 1 + Y Y = A 0 cosω 1 t + A 0 cosω t Y = A 0 [(cosω 1 t + cosω t) Y = A 0 ( cos ( ω 1t + ω t Y = A 0 cos ( πν 1t πv t Y = A 0 cos ( π(v 1 + v )t Y = A 0 cos ( π(v 1 v )t ) cos ( ω 1t ω t ) ) cos ( πv 1t πv t ) ) cos ( π(v 1 v )t ) ) cos ( π(v 1 + v )t )

23 This shows that resultant wave travels with average frequency v 1+v and resultant amplitude. Amplitude = A 0 cosπ ( v 1 + v ) This amplitude varies in time periodically with frequency DOPPLER S EFFECT The apparent change in the pitch or frequency of sound due to relative motion of source of sound and listener is called Doppler s Effect as it was first observed by John Doppler, as Austrian Physicists. For example, when the train is approaching towards an observer at rest, the pitch of sound increases whereas the pitch of the sound decreases when the train is moving away. This effect can also be observed when a listener moves towards or away from source of sound. Difference situations for the observations of Doppler s Effect are given as, Case 1(a): When listener moves towards source at rest. Suppose, V = Velocity of sound waves in air λ = Wavelength of sound waves v = Real frequency of sound waves V 0 = Velocity of observer v = Apparent frequency of sound heard by obsever We know that Or, V = vλ v = V λ Now suppose listener is moving towards stationary source which emits sound waves. Then the relative velocity of sound w.r.t the listener will be V + V 0. Then for this case we may write Relative Velocity Apparent frequency = Wavelength v = (V + V 0) λ

24 v = V + V 0 V/v v = V + V 0 v V This expression shows that the apparent frequency of sound is increased. Case 1(b): When listener moves away from source at rest. (Same diagram with opposite direction of listener) Suppose, We know that Or, V = Velocity of sound waves in air λ = Wavelength of sound waves v = Real frequency of sound waves V 0 = Velocity of observer v = Apparent frequency of sound heard by obsever V = vλ v = V λ Now suppose listener is moving away from stationary source which emits sound waves. Then the relative velocity of sound w.r.t the listener will be V V 0. Then for this case we may write Relative Velocity Apparent frequency = Wavelength v = (V V 0) λ v = V V 0 V/v v = V V 0 v V This expression shows that the apparent frequency of sound is decreased.

25 Case (a): When source is moving towards stationary observer. Let us now consider a source of sound moving with velocity Vs towards stationary listener. The wave crests detected by the stationary listener are closer together because the source is moving in the direction of the outgoing wave resulting in shortening of wavelength. i.e. the wavelength λ measured by the listener is shorter than the original wavelength of the source (λ < λ) Now Suppose, V = Velocity of sound waves in air λ = Wavelength of sound waves v = Real frequency of sound waves V s = Velocity of source v = Apparent frequency of sound heard by obsever λ = Apparent wavelength recieved by observer For this case we may write Apparent wavelength = Orignal wvelength Relative distance travelled by the source λ = λ S λ = V v V s v V v = V V s v v V = v V V s v = V v V V s This result shows that the apparent frequency of sound is increased. Case (b): When source is moving away from stationary observer. (Same diagram with opposite direction of source) Let us now consider a source of sound moving with velocity Vs away from stationary listener. The wave crests detected by the stationary listener are farther together because the source is moving in opposite direction of the outgoing wave resulting in increase of wavelength. i.e. the wavelength λ measured by the listener is greater than the original wavelength of the source (λ < λ) Now Suppose,

26 V = Velocity of sound waves in air λ = Wavelength of sound waves v = Real frequency of sound waves V s = Velocity of source v = Apparent frequency of sound heard by obsever λ = Apparent wavelength recieved by observer For this case we may write Apparent wavelength = Orignal wvelength + Relative distance travelled by the source λ = λ + S λ = V v + V s v V v = V + V s v v V = v V + V s v = V v V + V s This result shows that the apparent frequency of sound is decreased. Case 3(a): When both source and the listener are moving towards each other. The apparent frequency heard by listener in this case will be v = ( V + V 0 V V s ) v This shows that apparent frequency is increased rapidly. Case 3(b): When both source and the listener are moving away from each other. The apparent frequency heard by listener in this case will be v = ( V V 0 V + V s ) v This shows that apparent frequency is decreased rapidly. Applications of Doppler s Effect: 1. Doppler s effect has very wide range of applications in different scientific fields and in daily life e.g. It is used in measuring the speed of automobile by traffic police. Ultrasound machine do their jobs on the basis of Doppler s Effect which are used as an alternative of x-rays 3. This effect is used in finding the motion of objects like submarine under water.

27 4. Doppler s effect is also employed in light waves which is used in space and astronomical research. 5. Radio Detection and Ranging (RADAR) is commonly used to detect the presence of any aircraft in the airspace and it is very important in civil aviation and military purposes. Acoustics The branch of Physics which deals with the study of production and properties of sound is called a acoustics. This term is also used to describe the way in which sound is recorded and reproduced. This subject is used in developing auditorium, seminar, halls, conference rooms, recording rooms of radio and television stations, good acoustic conditions are required for proper listening and recording of sound and for this purpose the loudness of each separate syllable should be sufficiently large and echoes should be just sufficient to maintain the continuity of sound.