WAVE MOTION-1
Definition
  • A wave is a periodic disturbance which propagate energy from a point in to another.
  • Waves transfer energy from point to another point without carrying matter.
CLASSIFICATION OF WAVES
Waves may be classified into two classes:
  1. Mechanical waves
  2. Electromagnetic waves
MECHANICAL WAVES
Definition
A mechanical wave is a disturbance which is transported through a medium due to particle interaction.
or
Is the wave which require material medium for transfer of energy from one point to another.
Example
  1. waves on a spring
  2. water waves
  3. sound waves
  4. waves on stretched string (e.g. in musical instruments)
  • mechanical waves require a material
    medium to transfer energy.
  • when a mechanical waves travel through a medium the particle that make up the medium are disturb from their rest or equilibrium positions.
ELECTROMAGNETIC WAVES
Definition
Electromagnetic waves are the waves that consists of particles moving in electric and magnetic field. or
Electromagnetic waves are the waves which does not require the material medium during the propagation of energy from one point to another.
-The electric and magnetic field oscillates at right angle to each other and to the direction of propagation
DIAGRAM OF ELECTROMAGNETIC WAVES
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  • Electromagnetic waves do not require a material medium to transfer energy.
  • They can travel through a vacuum.
Example:
  1. visible light
  2. radio waves
  3. infra-red radiation iv. ultraviolet radiation
  1. gamma radiation
  2. X-rays
WAVES FORM
-A wave form is a shape of a wave or pattern representing a vibration.
-It can be illustrated by drawing a graph of the periodically varying quantity against
distance for one
complete
wavelength.
TYPES OF
Waves may be divided into two forms , which are:-
WAVE
  1. Stationary / Standing waves
  2. Progressive waves
  1. STATIONARY / STANDING WAVE
Are the types of wave in which the wave profile is not moving
  1. PROGRESSIVE WAVE
Are the type of waves in which the wave profile is moving
TYPES OF PROGRESSIVE WAVE
i) Transverse waves ii) Longitudinal waves iii) Mechanical wave iv) Electromagnetic wave
TRANSVERSE WAVE
Definition
A transverse wave is the one that make the particle of the medium to vibrate in a direction perpendicular to the direction of movement of the wave
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Example
  1. Water waves
  2. Wave on a string
  3. Electromagnetic waves
– A transverse wave is propagated by a series of crest C and trough (valley).
CREST
-Is an elevation of the medium above its equilibrium state when a transverse wave passes through the medium.
TROUGH (VALLEY)
-Is the depression of the medium below its equilibrium state when transverse wave passes through the medium.
LONGITUDINAL WAVES
Definition:
A longitudinal wave is the one which the particles of the material medium vibrate in a direction parallel to the direction of the wave motion.
DIAGRAM OF LONGITUDINAL WAVES
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Example
  • Sound waves
TRANSVERSE WAVES
LONGITUDINAL WAVES
1 )The particle of the medium vibrate perpendicular to the direction in which the waves advance
1) The particle of the medium vibrate in direction in which the wave advance.
  • A longitudinal wave is propagated by a series of compression and rarefaction
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Where C = Compression
R = Rarefaction
COMPRESSION
  • Is a region of high pressure in a longitudinal wave.
RAREFACTION
  • Is a region of low pressure in longitudinal wave.
DIFFERENCE BETWEEN TRANSVERSE AND LONGITUDINAL WAVES
GENERAL WAVE DIAGRAM
  • The crest and trough (valleys) in transverse wave can be likened to compression and rarefaction respectively in a longitudinal wave.
  • Thus we may represent any wave by a single diagram as shown bellow:-
2 ) It consists of crest and troughs.
2) it consists of compression and rarefaction
3) It can propagate only in solid and at the surface of liquids
3) it can propagate in all type of media (solid gas)
4 ) There is no pressure variation
4) The pressure and density are maximum at comp minimum at rarefactions.
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Where y = wa
ve displacement
X = direction of waves travel
T = Time of propagation
0 = speed of wave
TERMS APPLIED IN WAVE
The chief characteristic of a wave are:-
  1. Amplitude
  2. Wavelength iii. Frequency iv. Speed/ Velocity of propagation
v. v. Displacement
AMPLITUDE
  • Symbol, A
-This is maximum displacement of the disturb particle from its equilibrium position.
  • The SI unit of amplitude is the meter( m)
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WAVE LENGTH
  • Symbol, (Greek letter ―lambda‖),λ
  • This is the distance between two successive points of equal phase in a wave.
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Alternative definition
  • The wave length of a wave is the distance between two successive or adjacent crest or trough.
  • It is a distance that the wave travels in the complete cycle.
UNIT OF LAMBDA, λ
  • The S.I unit of wavelength is the meter,m
  • Other unit in common use are:
i) nanometer (nm) ii) angstrom (Å)
NOTE
1 nm = 10-9m
1Å = 10-10m
FREQUENCY
-Symbol, ƒ
-This is the number of complete disturbance (cycles) passing a given point in unit time.
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UNIT OF , ƒ
  • By definition
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= Cycles/sec
= Hertz (HZ)
  • Hence the S.I unit of frequency is the Hertz (HZ).
1HZ = 1 cycle/ sec Other unit in common use are:
i. Kilohertz (KHZ) ii. Megahertz (MHZ)
NOTE:
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SPEED OF PROPAGATION
-Symbol, V
  • This is the distance covered by the wave in unit time.
V = Distance covered
Time
V PQMZCqAzruOiA8kCV VfD93fAo8SG51vgfxFUm4NpEYk7rafhUgcSEtVZO9BySNIGlzKqHC1i1OHx3JY0GLEXb ZcllMWiQtxpcVLnhe2iRUE5ajWU1dTpp9WP 0PUPfN6nZz2g
UNIT OF V
Definition
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-Hence the S.I unit used is meter/sec (ms-1)
PERIOD
  • Symbol, T
-This is the time taken for the wave to make one complete cycle (oscillation)
  • It is the time taken for the wave to travel through a distance equal one wavelength -The S.I unit for period is the second (S)
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RELATIONSHIP BETWEEN ƒ AND T
-From the definition of ƒ
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-This given an alternative unit of ƒ i.e. per second (S-1)
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RELATIONSHIP BETWEEN V and ƒ
  • From the definition of V
V = X
T
For
complete
one
cycle
x
then
t
=
T
(=period)
v
=
λ/T
But
f
=
1/T
where
v
=
λf
v
=
velocity
λ
=
wavelength
T = Period
PHASE OF WAVES MOTION
  • This is an angular displacement of a given wave particle in time t.
  • This term is usefully in comparing two wave motions.
  • Two waves are said to be in phase if their maximum and minimum values occur at the same instant otherwise there is said to be a phase difference
Two wave in phase;
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PHASE DIFFERENCE / PHASE ANGLE
  • Symbol, Ø
  • This is the difference in phase between two wave motion
  • If the phase difference is radians then the two waves are in ant phase (out of phase)
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EXPRESSION OF PHASE DIFFERENCE
  • Consider two particle O and P along the path of the waves
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  • Let O be origin of the wave
  • A particle at P a distance X right of O will vibrate in different phase with the particle at O. – Let Ø be phase different between O and P
  • Now
2 rad Image?w=77&h=23&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
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PROGRESSIVE/ TRAVELING WAVE
-A progressive wave / traveling waves are that wave in the wave profile move along with the speed of wave profile across the medium
– Both transverse and longitudinal waves are progressive wave i.e. the wave profile move along with the speed of the wave across the medium.
-The oscillation of any progression wave repeat at equal interval of distance called wavelength and at equal interval of time called period.
-The vibration proceed to progressive waves are of the same amplitude and frequency.
THE PROGRESSIVE/ TRAVELING WAVE EQUATION
  • Consider a progressive / traveling wave which is moving from left to right with a velocity V.
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  • Let O be origin of the wave
-The displacement y of the particles at O
  • If the wave generate travel from left to right then a particle at P, distance X from O will lag behind the particles at O by a phase angle Ø given by
Ø. Image?w=61&h=34&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw …………………………..(i)
  • For the displacement y of the particle at P we have:
Consider the particle vibrating with Amplitude A
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Y
is
a
displacement
t
time
t
Sin
θ
=
y/a
y
=
a
sin
θ
But
θ
=
wt
y
=
A
sin
wt
This is displacement at time t when initial displacement is zero. But if initial displacement is y’ =
A sin Φ
Displacement y = A sin wt + A sin Φ
y = A sin (wt + Φ)
Substitute equation (i) in this equation
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Where
A = Amplitude w = Angular velocity t = time
Φ = phase difference
If the wave is traveling in the opposite direction i.e. in the negative X – direction then the equation becomes
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If the wave is traveling in the same direction i.e in the positive x- direction the equation becomes
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T = period
Problem 01
  1. What is a wave?
  2. Y = A sin EvhRadkeTqWsR2p4cqpff4Frglynr9SxQEZAdJnBHM1xh9Z1gGjQxz4TWYFaueOs4v36dl GnvqK9 5yqPzIKa S5sQgifFPVu O06xOusyu0qPaHz01ngGRvTAkSTiKBbcOv6Uis the equation
Of a plane progressive wave where x and y are in cm and t is time in second.
Determine:
  1. Frequency
  2. Wavelength
  3. Velocity
Problem 02
A certain travelling wave has equation
Y = A sin (2D27LQI3un6D2gaIc465iGhMiMszauN5kMhzSESJyxBH1zqL14y1Po2 Oo Fg1XPz08QHZAvQmfjw5QKzGIPWxdCTh7jsL G0oU4Mr669NqQUdPNZXn2HTSJXOIiZxGao4nxiYkt + kx)
  1. Deduce whether the wave is traveling in the positive or negative x-direction.
  2. If 2D27LQI3un6D2gaIc465iGhMiMszauN5kMhzSESJyxBH1zqL14y1Po2 Oo Fg1XPz08QHZAvQmfjw5QKzGIPWxdCTh7jsL G0oU4Mr669NqQUdPNZXn2HTSJXOIiZxGao4nxiYk = 6.6 x 103 rad s-1 and k = 20m-1 calculate the speed of the wave in the medium
PATH DIFFERENCE
  • This is difference in path length between two waves which meet at a point or between two points in a given wave.
  • It is the distance corresponding to phase difference
CASE 1
– Consider waves from two sources S1 and S2 which meet at point P.
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Path difference, ∆x = S2 P- s1 p
CASE 2
  • Consider two point P1 and P2 in the path of the wave from source
S
Path difference, ∆xWy DlIOv73UKnydQpc2PmBcXbdgmc3B4aXgdsHKMNmjTOloDn5KpuAfKynNJfkAvvjBrQq6GBJSDfPPy5WooiGXzjhEjS0ovj8eUloPhgm6AYGQ38ftc Ns9v1taJYiuqTp7QM
  • from the expression of phase difference
Ø = 2πx
λ
  • when x = ∆x = path difference, Ø
âˆ†Ø =
∆x
λ
Problem 03
A train of plane wave sound propagating in air has individual particles of air executing simple harmonic motion such as that their displacement y from equilibrium position at any time t is given by Y = 5×10-6 sin (800πt + Ø)
Where y is in cm t is in second and Ø is a phase term. Calculate a ) the wavelength of the wave
Given that velocity of sound air = 340ms-1
Problem 04
The speed of wave in a medium is 960ms-1. If 3600 waves are passing through a point in one minute, calculate the wavelength.
Problem 05
A progressive wave of frequency 500HZ is traveling with the velocity of 360ms-1. How far apart are two point 600out of phase?
Problem 06
A plane progressive wave of frequency 25HZ, amplitude 2.5 x 10-5 and initial phase zero propagate along the negative x- direction with a velocity of 300ms-1.
At any instant what is the phase difference between oscillations at two points 6 cm apart along the line of propagation?
Problem 07
The equation y = A sin (68dtyZsQLI2j HPML6ATx1hRkDYzuZFbByv8nQDd12y7ehnuekxg7hwsOyzc8YA0JKVdpmrar93mHFmvAWfZLUzdnqACxdHuPr0vIDEy9bYW1kthaQjMGlGWSDQlXsri33hzESw represent a plane wave traveling in a medium along the x direction y being the displacement at the point x at time t.
    1. Deduce whether the wave is traveling in the positive x- direction or in the negative x- direction
    2. ) If a = 1.0 x 10-7m, XDzX2lKdCa4uhTWI YDLqkGLykTMqgoW5TzIM6zNd8ZJc2axssww0IlPXcOkdcUTrzgsxBRi H 4eUf6zPj8 P6 X4oTowF5dVEPC4UwZY WucXpo3GjHW3MizoOGV SM Tnot8x 103s-1 and k = 20m-1 calculate
    i) The speed of the wave ii) The maximum speed of a particle of the medium due to the wave
    SUPERPOSITION OF WAVES
    • The principle state “If two or more wave arrive at a point simultaneously then the resultant displacement at that point is the vector sum of the displacement due to individual waves”.
    07dVKsSB68Qk7IEqLFfYU3sUOevbeWxfgVYbRC28wsFuw3cCBHTIOOZtKFm5NmfsvN3foR0gKqQYTH8oFvkSxJh5PeJ5ti3RB5LXqc2nQN 65bzf7pnx8YJUkdoR2I0dmZ7XTRg
    • Where y = resultant displacement
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    Problem 08
    Two waves travelling together along the same line are given by:
    Y1 = 5 sin (Lm32ompYhU5InAd3co OPD2THzY8adSfvuYgTVHwvgJIqYAbOcHvwXelj2vyhsXsiHWVYwOm5p6kiN44D7WdCUzSi4 Dzs AxOhHrCO16Yt1Pyc 7RpcqMagt7j QqYLzeowwwY ) and
    Y2 = 5 sin (TW9 HD6tCs9 Ioln Q1fJzcXd0mRR9Bur5zgLXs2C42nus9kf6FG0leSLFMA3uB5lbdUQQycyJ9AGqji J V5 WNF01YQipzlCVC4OIZQ2saRzDi Ybaky86b1CqpKFJf3 CZ3g)
    Find:
    i) The resultant equation of motion ii) The resultant amplitude
    iii) The initial phase
    angle
    of
    the motion
    IMPORTANT CASE
    – There are three important cases:
    OF
    SUPERPOSITION
      1. stationary waves
        1. beats
        2. interference
        STATIONARY WAVES/STANDING WAVES
        Definition
        A stationary / standing wave is a form of wave in which the profile of the wave does not move through the medium but remains stationary.
        HOW A STATIONARY WAVE IS FORMED
        -A stationary wave result when a progressive / travelling wave is reflect back along its own path.
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        -The incident and reflect wave then interfere to produce a stationary wave
        -Thus we can say a stationary / standing wave is formed when two progressive waves of the same wavelength frequency and amplitude are made to move in opposite direction in the same medium.
        -A stationary / standing wave has two important points:
        i) Nodes( N) ii) Antinode (A)
        NODE (N)
        • This is a point of minimum disturbance in a stationary wave system
        ANTINODE (A)
        • This is a point of maximum disturbance in a stationary wave system
        THE EQUATION AT STATIONARY / STANDING WAVE
        – Consider two progressive waves of the same wavelength, frequency and amplitude to be moving in opposite direct within the same medium such that when they meet a stationary wave is formed.
        -Let the waves be y1 and y2 such that
        Y1 = A sin (2bxg Oo6FC1auAyZURn42KxYFM4mMyKxFtZ UXYgeE5z J7HofztRTWCpNWOiRKARMVAmWW44kb504X7NawLQIeukjug9tWxVgIg0XP 8JFNom2ETEZ52xI5ubmO96eydPScNxM
        Y2 = A sin (68dtyZsQLI2j HPML6ATx1hRkDYzuZFbByv8nQDd12y7ehnuekxg7hwsOyzc8YA0JKVdpmrar93mHFmvAWfZLUzdnqACxdHuPr0vIDEy9bYW1kthaQjMGlGWSDQlXsri33hzESw
        -According to the principle of super position of wave the resultant displacement y is given by:
        Y = y1 + y2
        Y = A sin (Image?w=185&h=27&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
        Y = A (sin (XTj4wFxXtZ8D0wrcDSkjWmSMKE9p9x5jQ QgBYZLqNk7eY3hEhCYDj08WVPoFOXI8L9OIuOSs9foaOUCqUqK8jhozxcf 3aTYrqQqTr8ue5Ld7UD J3d7UWbY8Z3 HwsCvdqQT0
        Y= 2A sin (Image?w=320&h=27&rev=1&ac=1&parent=1LROdijXKcU8Ys2KKp6YZtwhvOKDJrPcw
        2 2
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        PROPERTIES OF A STATIONARY/STANDING WAVE
        1. The distance between a node and its neighboring antinode is one quarter of a wavelength
        TjUkD 4sMOgzTo28M67bLIvEYFkIV9YSGEpt61ROym4jWM8gfeDU6MWt QhFcks I0k5aoS2eXfcOCGhOazPjYHaVG AKjkb3vCQ2eFQDERbze5lgHoxqOUHejUKftDGYJ3ZY8o
        1. All point along the wave have different amplitude.
        2. Point between successive nodes are in phase.
        DIFFERENCE BETWEEN PROGRESSIVE AND STATIONARY WAVES
        PROGRESSIVE WAVE
        STATIONARY WAVE
        1)The wave advance with a constant speed
        1) The wave does not advance but remain confined in a particular region
        2) The amplitude is the same for all the particles in the path of the wave
        2) the amplitude varies according to position being zero at the nodes and maximum at the anti nodes
        ) All particles within one wavelength have difference phase
        3)phase of all particles between two adjacent nodes is the same
        4) Energy is transmitted in the direction of the wave
        4)energy is associated within the wave but there is no transfer of energy across any section of the medium
        Problem 09
        1. Explain the difference between progressive waves and stationary wave
        2. Progressive wave and stationary wave each has the same frequency of 250HZ and the same velocity of 30QzUhqSc9iK41wO2aACRoVZD59tpf ZZnVg8as6AZr40ylj Xgn3l39jEsnCoQvle1V36Es03L4bXDnOXWuacqC PzKpmYQvHGl49ZuDUxLj8CpQeSVv FzGMqH6Gm6Xkzfd0sFA. Determine
        (V0nHBnJxQh5raMCK4B4lnC20RcVuMD IxmOYFl7SrpcCIEZH6xV5Rn1QUxb0 ZZN48zRBzq2yswVWOCgzc Yrym QpuZ H Am6nkB ECeEQXn40k6HIi2vroaquBWkA9SNskt1oThe phase difference between the vibrating points on the progressive wave which are 10cm apart
        AblKZV4ifLkqJ3mZmrfX7Y8K84 Qv4dTTsRyfqduJugce8Fvfm0bXC8hx3kfkwPGIAMvt3Jb7wPC5TWcVzDSU ZDIgkUernlj6M5K5yvLaeEknWMMWPCZ5zaDbHZNfx5RzwKTCUThe distances between nodes in stationary wave
        (iii) The equation of the progressive wave if its amplitude is 0.03m
        Problem 10
        Two waves travelling in opposite directions producing a standing wave. The individual functions are given by:
        Hr6heKGWfArCFYccYG ZV6BNfxqtOkwWUEToxKWX8eZc5EDFraOqA2UYgh Lm59kONHSVwSwntgRrBLu504lgNo96jLHmtRRJLv88bt3sOyOSSO5EvWZrhe805c1PNkAtMNl Fk
        JWiPm SD AXuej2VsCFpj H1i5zAOJm7F9epm0Q KjpOP5Pl4cITIB2OOgiQ5yWQpq0zJWcGVGmoA9PYmKanTmUgE Y6cUPs99z5XXlVAym7qocvBxBFUSgQKlrHvozcURzonvE
        – Where x and y are in cm
        (9gICk0y1Ea5Zml6jRaDM UAiIKKnqW8nWzR1FXJM CYIAewJ3c5WWWKR6MMiHdH SJReG3S4GFFWQUbItPZ2efLPewFtfJCB74zZyV4kjvzNHLBuevOvHZbF7xRNbjTKvXHuGasFind the maximum displacement of motion at  VFYtLwmZcxt3kB8LeMOl GV NIkXwN60ewW640gS2Zuu0GrTJgFN9L DjMpi5JZ88UXq6S2ZTR5uGiSDj3HmlriHvpubf8Qc G3RJ LvnkeYZfro54boUhA7gtPaDJyWZQqk
        (V0nHBnJxQh5raMCK4B4lnC20RcVuMD IxmOYFl7SrpcCIEZH6xV5Rn1QUxb0 ZZN48zRBzq2yswVWOCgzc Yrym QpuZ H Am6nkB ECeEQXn40k6HIi2vroaquBWkA9SNskt1o Find the positions of nodes and antinodes
        Problem 11
        The transverse displacement of a string clamped at its two ends given by:
         5VkxHWqrLeVEk8HDPCpM5jnA 0j9fnXv7QvlCI OQ6Qj2lMW2GVtbR JKhnhphV91D QwqqC6ueWGPmXnVo0eXIqncHp Mwd MH8cUfHkLI4dnRKSmh5lkG0xLYpF S4XoKS0A
        Where x, y are in metre and t is in the seconds
        (V0nHBnJxQh5raMCK4B4lnC20RcVuMD IxmOYFl7SrpcCIEZH6xV5Rn1QUxb0 ZZN48zRBzq2yswVWOCgzc Yrym QpuZ H Am6nkB ECeEQXn40k6HIi2vroaquBWkA9SNskt1o Does the function represent a travelling or stationary wave?
        (7ZNzmkHq7HZGNdx9u AytCpNm9UAt8bSqQ8XwCq13xyzZ QQZ43RbkqUV0Hl5AJGT2Bqbc6OeMx9J2B6RYthsy09cLMqa4gVd2IzGpv1XTpOOOA2NnVwlxB0iYoe2lvQAyld6YQ Interpret the wave as superposition of two waves travelling in opposite directions
        What are the wavelength, frequency and speed of propagation of each wave?
        Problem 12
        A standing wave on the string has nodes at 3h4QCHtp J1zREff9ULNrwTO44tSWmkX3UnV7fpCDM NcBE R3ncUwlCgRf F3L8CM0iDeKHLx5i HVBKn23no2XwunJiziPv7oJjxLLMVES9KsjFNhsYrhTQ2SZVc1NaXzll6AWhat is the wavelength of the travelling wave?
        Problem 13
        The equation of standing wave is given by
        ZFmV4bdRpAMO3Gm3drASyX3wPO3Zbec4Uwcx30ouZ4JqWiskUPUB 7 AWAe9xJBqlhmSiHzhFnhozVDdkRmQMJauMbHE5elig76l2Dk7a2s1HKYaIDXJQfUwUOpXh4tKhL GhKY
        – Where x and y are in cm and t in second
        Find: (9gICk0y1Ea5Zml6jRaDM UAiIKKnqW8nWzR1FXJM CYIAewJ3c5WWWKR6MMiHdH SJReG3S4GFFWQUbItPZ2efLPewFtfJCB74zZyV4kjvzNHLBuevOvHZbF7xRNbjTKvXHuGasFrequency and wavelength
        (QSRVg69OOzH3wz2ypTQYq01fn J6r7DlTG0Cf9KSUG88UMWfGtDXoyCOkn1HC8cOdW13lHUU1MfMEBLm5v4vuvznZk80hyzC8O20deen9UQbmCNbIb6 GpPHRNkiNWfWw56BdAw
        SOUND WAVE
        Definition
        Sound is a longitudinal wave motion which is conveyed through an elastic medium from a vibrating body to a listener.
        AUDIBLE RANGE
        -This is a range of frequency which can be detected by human ear.
        – The human ear is very sensitive and can detect very faint sounds.
        -The human ear can detect sounds in the frequency range of 20HZ to 20000HZ
        -With increased age upper limit of frequency range fall quite considerably
        -Howev
        er, the ear is most sensitive sound with frequency around 3000HZ
        INFRASONIC SOUND
        -This is a sound with frequency below 20HZ.
        ULTRASONIC SOUND
        -This is sound with frequency above 20000HZ.
        -Some animals including dogs, cats, bats and dolphins can detect ultrasonic sound with frequencies‘ as high as 100000HZ.
        PROPAGATION OF SOUND WAVE
        -Sound waves require a material medium to be transmitted through.
        • It cannot be transmitted through a vacuum.
        -Sound is transmitted by vibration of particles.
        -One particle vibrates to transfer energy to the next until the sound reaches another point.
        • If the particles are closer together, sound will travel faster.
        • Hence sound travel with different velocities in different materials.
        IN SOLID
        -The velocity (v) of sound in the form of a rod wire depends on:
        3psrK92Dj0xfGRr 951HNWA KHnI F7M6cXJadKyvGjTc5qG1uIDDExq3Qe0xmw65QkFc7365adzKfYCNXfUVoXCdv53kylbY5WIYoXtqEt1U7bg5jV2A4JzyYbTDZcgvfkPAyg Young’s modulus E of the solid.
         8xXGdIFcL2nXlHbZkO9ITl5phzIUCl4XirJlkLPBzv5l5stWfVkJ4XlcISNE NTKXJvWeKDcjjwmlgagVhjnTFgP8tCHiSsrTV4G 5nAvwCAhShrudIgkkkR82BGIWN31yQWHg Density UA RBHr37K9OvQwLxD9DDj7oE26Oj2uY0yPUDtuauBBxtbU TMsHVjumh6VYNPvucuKjt9us3zWLngrp1T7H6x2CeuYgGbA1MI8istCHWS6W3vIWSclRujcnP1NYVuuhd9lJxo4 of the solid.
        -One uses dimension analysis to get relationship
        DzWh3fZv88mZ4DsO NOVKZG6f 5Uh8BNySudAifi 8X YW TWenzp 7ZdXNYwZYiV3UdnlDpbjHOqJPodJBMyCtu7rax0FcWckKg6V1OPUWgGWEo5Q RcU55ySK2i4H734 Wb4
        -Which gives
        4qz8YkPfull2dHM6a KROyen6CxLvO 772B6TPpLfsrs0O 2 0i0icNSDTAp5POXnFbpFyqsvRLkBSAqIUtz71uRVhGGxjbA LYt2P8HX6XolZQ BnHo6Dl40rBHI10qkqH65gM
        IN FLUIDS
        -The velocity (v) of the sound in fluid (liquid gas) depends on:
        (ROtOu76Hf4KIJG5pGuq Vfhl6fr9cYFWymCSc MAQEu7m7zrLq3nkL3Af2IZ8lPmFMDYi2tjWnYm5f2s5ojJ9h5nJRUF2kxRo 0gK3s5M BmZmVmGlUTyitcQBXxW4miiy7nXuQ) Bulk modulus ELyzbFPSR494 0ZiaxMKZ64Bqb5XHMFiOjKxMZBfPt94sQkF2dygjcBQUZck8UFKpe HW G9IdA88sGIKFHImvBrqom8lMDuYShCQNQz RDbFg OiA9EQZ4xaYI1200I23lYwjY
        (RrYaWnYNrf9KKT LWeG4oV6NOxFqDbHS5hOXJdxjE7fSI14pW5KMI JKVP5taOcXWytvcvqsPGFVdV5uRyphTJQCg0eMh6Gttijky3oLklhw 3DL0ic5bqkNqWPNwHiOTB0APZk) Density UA RBHr37K9OvQwLxD9DDj7oE26Oj2uY0yPUDtuauBBxtbU TMsHVjumh6VYNPvucuKjt9us3zWLngrp1T7H6x2CeuYgGbA1MI8istCHWS6W3vIWSclRujcnP1NYVuuhd9lJxo4 of the fluid
        – Again we use dimension analysis to get relationship
        VarO2c5fTCC8p1f99A4I LXGAesOGP1jqqEH8aWZ9M7bcT8xGcNRTYfkkomrVJ3EFEfyBEAAYBVz0w2sQzIVOTd21AW3nju73NKLmPB5l1p2SKLZopMMRULmkKYjpbWJeQikDCU
        NEWTON’S FORMULA
        • Newton assumed that the propagation of sound in a gas takes place under isothermal condition (constant temperature condition) in isothermal conditional Boyle`s law applies and hence: PV = K differentiating this equation:
        2cBXP9gVPLkjeo YU LcVw91X 8iTYyy RHmcHvwcAaHvAy31Q3zlqiQc10 IOP2eljJFyjtIQeNOZD4AquCfL06xGNhMYjlGEOYptPvz1BvLoTv7dld 8b44T5V7rdFLAgJBsk
        T 5nAImZdpzuv3hAN JcjVb8tQumAEEAwiCo6MSQ5kevkpDbbfIoZIQU5 DVwJiZBXbYj5jX3RLLNIwtNToClyUuLgjPHRFpzNKBB2Dtf4tAK YfzyWHQ VxWlpA6wc5XHMdamA
        8tIkmLIfwwJK5cCs64tkNodnnuFjmvYu2ZD2g8pIkZgCHnCjcfhOB4oh4ZbBTrHAjDGStvVUmJJlp0jRZMLv1o8C0PY01 V6ADjBmUdxoHtImOa3UfPtBUbofU Vmz LxaHkuyQ
        JWcv1slpkZeSW3ZQU3nsyQd NMgvgoMKtgSfrlQ5eU0LTvJ5 CpNXEo70v8Bnang4dzASDcZzng4sYVZA 6s8TSy2jd5WjKqO1nOYd IXJiM1 A4I0OXhd2VuAdRNwPvn4 Mpfc
        • Where NkZJYfMrI ZwOGQKjWx9qv5Epq26m9Do6wihiOGeqjEH6gCOYbPh X5Tcc5Z3ocrqzLboXRECEB4vije2fq5F JAppbGXRSIvvrgpYHiK 2L4A5WW6teLIEEOwRD9ynud2Cr3hw = change in pressure
        HfFvgK8l 1dWYd69mMOavhSL4NonzxwoW2wK8TRe YtyxqZb MQFui6grN0UDt QoMwhUoNkmmGioartO5Gz0APTXZfDCc6GI8SRNRM 0WGPkUv YIyOXYMcK6nUsQ K8rOmrYo
        • By definition:
        C7LeWNkg UIDgsEj4OKveUvZVdnWtHhMrMc8JFqUSQRz3U5BQOynT4iamM IbOpzb9a 4JFWb7I50 M ZqQdqIClFlzA7FSKTLwjmqCjoc IHgQt30PvRMpgE9oxTnvStgsLLWU
        Under isothermal condition
        RKTAZm3GKYqlZUh PYAgppfKi4junCauqb3oz2NcfqfvrBwl6O3KTea4AO 9r GAHLCjkrjqKulFeOgPtRBRRMH0ow3BJ5NsAb3wJkJPk6TNKbVfyNupdy XJftnJr 11VK7kyc
        From the expression of velocity of sound in fluids:
        G39SJuCT AuqCrbtB7DAbFMrMdBV4t9Mwam9pfRhngxirE8gj4I4stqv1Qxpv61tK5a3ITgqK Wafrjq2qXduRBh9RMh2nJmgNA B9B 8UGspyCiHpiqBYDp 1tbrqKgwSTBFc
        OVe9XMcXLxbBy84MDFD Kf34V3cgkZECE8nALOHRD3kUYNTazC5o3giRrx26tKz43CixUPn 2sqRgGa H JS1kash 2UGsWUPDPu9 1HIHsAfn NpR8xxAuCEU3fItaRWNoCcIs
        Applying this equation to the case of air at S.T.P
        Given
        HahQZmEfLSGjSgBJH9Gp262pJsYdFaRWCZ0wOtT3BLlibqpGcli Rnr DZme5KFpCFxDShpfqmPUVisJbAqQDmxAPL8j6K8RDPUfrRG19RHsiuje B3V7zoKaiEpzDy8zHxJHdM 1.013 x 105Pa
        KVTQsdwwPK00a8HKRcN23G7VNmaAymDow XufphPbOhw 0gxVNkgUh WXBHE0XoM70 TM25NEWIgzfx4gtzo URjeKFB3dH X 3OL7Ql70 Ey2Gi Sm1rPEwI3QVaDpWtGe1weg V = 280ms-1
        -This value is less than the actual value, which is a about 33oms-1
        -This large discrepancy shows that Newton`s formula is not correct.
        LAPLACE`S CORRECTION
        • Laplace pointed out that Newton`s assumption of isothermal propagation is not correct.
        REASON
        -The compressions and rarefactions follow each other so rapidly that there is no time for the compressed layer (Which is at a higher temperature) and the rarefied layer (Which is at a lower temperature) to equalize their temperatures with the surroundings.
        -As a result the sound propagates under adiabatic and not under isothermal conditions. LAPLACE` S EQUATION
        -Under adiabatic condition of air:
        Of air NohEZQpTTLUJWppJ3BBtxLP AFHplfp7zGSysMYc6PwnFCfNkPNFsuyUGSDFQ3PmMXTmXTj WOVSpg PgDISCgo4bwq1niIdFzvgHo8eu7uhMJC4R0g N8Z VNCyy1PNNVqWjgconstant
        UZJ7PCyfLgZtIA2VAJ6zNwnjviRCJHd0 GpCCBG1QDLVif5H OxSUcSw1qPeD2cblmFeQYx1CH XnF XV CaGR9oehHUcPNDHn9XVoNlLUpdr4MW8dLWArxLkC EZiuOT176qc0
        Where
        E6ZniF8OXvg MhkcL3Vxc M6ab0Rs4zov4P0gHWdQRxkXrgM6X3KP7mpPIdlVQTdBffeWX2qpTzS8vxTV6Aa2apkyz6izVbNn HYXz3wNNpY42iRCC6FKgZu254s4Fpsvt6h6Cg
        FNOI1k2r0Y7f2S5q3uEJzDt1KV8Fa8nw91T3dhHt1awjY2Q OMteQxhRVpqusLOtVdAJaH2idYumaUTBR8g38p 6uFosRFNdTWXQXq22HCYlnAVofGbU6W2Dv2dim9SInitCYuM
        HAPsfhIxta5uRVfI7PuEiD01D2ENI7J WQXXAVgjZzKYuqw4 FiYyUwYc C2w4 VfN9EU0K Xq5P8vO R3cmnHwn1GaBHRGLwzefchG23q8R RvDj7YxSqfg00E0b8NcJgzH528
        MLqrOxnAl6q CM8k7C5FX2JPd5dWR812f2hwbCw5Dwij3 O0968QOFr0WXwfuz OaPXDSx LpmPTX941TcvMLdfdVjRN4NgGpGK 0DY0x19BxFYF Gpn0mCbIZJEsZ3HqwRVJwQ
        Differentiate equation (i) above
        ZJomc8IbHWu1J5QJGtkIjF Nr50trz3HYA8M4bjt05w5SRV0wnWGXuHqBRUo8TpLqgyMtNxEkPG5TiM2Uv3NQJtr4sctXPqKYZ3ahmYwNTLXZ 04aQZkjdQO3MjCxel2xMQWDyc
        PRvwBypSCaNPVHXdcVeak8Oes1uKoRsqhDpUOPlqgZcMm6WmKfi1zEfm ZZwjTB4Fdg9NUsqq88 Vs76CJ2Zv51nORd4k7 G4MpE9wo8ZXS1wlHzjZIFvzGhyDYvzHy4UB04 PMs
        7GXxYn7e8c X228CKUQsMAqTZl2EF3HDSKgNUkZBLFpWD93pmXnDdhb2jutDDEbiV Ko7dsXKDcyL4793bISnhcESqp6hx06dttOMeepV7IcnqbDIsyUEk294lcDO7Qn8D24Iss
        Z8cW0yNYO1X MnfwKS4y9 JpjacDgv8G TMf0fOICq9CQvBhry3FEBzc YthtIcjGKjfw8 Qn4n0PfHjarbuZvOoF3tKdpUsGEIj O8IOx781h0zx6mJkeG5tS6nt2kWy8OKocY
        Under adiabatic condition
        N4ZeaQSh 6mDsdAO5YfXIHRZO30r9pjsxmKwSB720hmIiofZuNC53oPSkHNo NkdcEjHb0GVI UhO2ZMFgK TpCoYSZjhElyXs1aj4 GfW32QcTIwgmO1Tdn1C 4TvAV40GSnMw
        From expression of velocity of sound in
        G39SJuCT AuqCrbtB7DAbFMrMdBV4t9Mwam9pfRhngxirE8gj4I4stqv1Qxpv61tK5a3ITgqK Wafrjq2qXduRBh9RMh2nJmgNA B9B 8UGspyCiHpiqBYDp 1tbrqKgwSTBFc
        8rAQU OXaTLXHgzx1lT5ix4OZQQJ0x FO NqifXoJgZcCb FmQjw6UKBex8zDGtqTGLSVXjaZeJfs0oR2OJR3HJrndqjaNaYflZafdB5qMFPpajmQ0mYmzFnjQh8X83TnOL Ju8………………………………(iii)
        – Applying this equation to the case of air at S.T.P.
        GIVEN
        V = 1.4
        P = 1.013 X 105Pa
        P = 1.29kgm-3
        V = UI1fbTbnfwVNOq7eaMei 4EReDVEKWm6oFThyjoS53lwNcgyxIBE6OLrxuWkypAJc1MBSk Rof1Jnaouhaha6FdJqxGq4bLeClppoj3owM0knFaDx0HSIOb99lmp XhRoMKYrdw
        1.29
        V = 330ms-1 which agree with the experimental value.




        ');}
        Bc0138c3d2dab0944d91d638547c2715

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        2 Comments

        • C3d744c86b4e65aefd353f89dee9a64c

          Kay Tee, April 2, 2026 @ 2:16 pmReply

          It’s awesome

        • Ce24c0fe4a34297b7d5847768de7bacb

          Oliver Kanyesigye, October 28, 2024 @ 10:08 pmReply

          Good notes

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