MULTIPLE CHOICE QUESTIONS I
Q.1. Water waves produced by a motor boat sailing in water are
(a) Neither longitudinal nor transverse.
(b) Both longitudinal and transverse.
(c) Only longitudinal.
(d) Only transverse.
Ans. (b)
Solution.
Water waves produced by a motorboat sailing on the surface of deep water are both longitudinal and transverse because the waves, produce transverse as well as lateral vibrations in the particles of the medium. The water molecules at the surface move up and down; and back and forth simultaneously describing nearly circular paths as shown in Figure.
As the wave passes, water molecules at the crests move in the direction of the wave while those at the troughs move in the opposite direction.
Q.2. Sound waves of wavelength λ travelling in a medium with a speed of v m/s enter into another medium where its speed is 2v m/s. Wavelength of sound waves in the second medium is
(a) λ
(b) λ/2
(c) 2λ
(d) λ
Ans. (c)
Solution.
Frequency remains unchanged in both the medium.
So,
λ1 and λ2 are wavelengths and v1 and v2 are speeds in first and second medium respectively.
So,
Hence the wavelength of sound waves in the second medium is 2λ.
Q.3. Speed of sound wave in air
(a) Is independent of temperature.
(b) Increases with pressure.
(c) Increases with increase in humidity.
(d) Decreases with increase in humidity.
Ans. (c)
Solution.
We know that speed of sound in air is given by
for air γ ans P are constants.
where ρ is the density of air.
⇒
where ρ1 is density of dry air and ρ2 is density of moist air. Due to the presence of moisture, density of air decreases.
As
Hence, speed of sound wave in air increases with increase in humidity.
Q.4. Change in temperature of the medium changes
(a) Frequency of sound waves.
(b) Amplitude of sound waves.
(c) Wavelength of sound waves.
(d) Loudness of sound waves.
Ans. (c)
Solution.
Speed of sound wave in medium Here γ, R and M are constant.
Hence, v ∝ √T
(where T is temperature of the medium)
It means when temperature changes, speed also changes.
As, v = fλ, where f is frequency and λ is wavelength.
As frequency (f) remains fixed, v ∝ λ or v ∝ v
Hence wavelength (λ) changes.
Q.5. With propagation of longitudinal waves through a medium, the quantity transmitted is
(a) Matter
(b) Energy
(c) Energy and matter
(d) Energy, matter and momentum
Ans. (b)
Solution.
A wave is a disturbance which propagates energy and momentum from one place to the other without the transport of matter. In propagation of longitudinal waves through a medium leads to transmission of energy through the medium without matter being transmitted. There is no movement of matter (mass) and hence momentum.
Important point:
Characteristics of wave motion:
Q.6. Which of the following statements are true for wave motion?
(a) Mechanical transverse waves can propagate through all mediums.
(b) Longitudinal waves can propagate through solids only.
(c) Mechanical transverse waves can propagate through solids only.
(d) Longitudinal waves can propagate through vacuum.
Ans. (c)
Solution.
In case of mechanical transverse wave propagates through a medium, the medium particles oscillate right angles to the direction of wave motion or energy propagation. It travels in the form of crests and troughs.
When mechanical transverse wave propagates through a medium element of the medium is subjected to shearing stress. Solids and strings have shear modulus, that is why, sustain shearing stress. Fluids have no shape of their own, they yield to shearing stress. Transverse waves can be transmitted through solids, they can be setup on the surface of liquids. But they cannot be transmitted into liquids and gases.
Q.7. A sound wave is passing through air column in the form of compression and rarefaction. In consecutive compressions and rarefactions,
(a) Density remains constant.
(b) Boyle’s law is obeyed.
(c) Bulk modulus of air oscillates.
(d) There is no transfer of heat.
Ans. (d)
Solution.
Q.8. Equation of a plane progressive wave is given by y = 0.6 sin 2π(t - x/2). On reflection from a denser medium its amplitude becomes 2/3 of the amplitude of the incident wave. The equation of the reflected wave is
(a) y = 0.6 sin 2π(t + x/2)
(b) y = -0.4 sin 2π(t + x/2)
(c) y = 0.4 sin 2π(t + x/2)
(d) y = -0.4 sin 2π(t - x/2)
Ans. (b)
Solution.
Reflection of Mechanical Waves:
When a wave reflects from a denser medium, there is a phase change of π.
Given equation of incident wave
yi = 0.6 sin 2π(t - x/2)
Equation of reflected wave is
yr = Ar sin 2π(t + x/2 + π)
Amplitude of reflected wave
So, yr = - 0.4 sin 2π (t + x/2 )
Q.9. A string of mass 2.5 kg is under a tension of 200 N. The length of the stretched string is 20.0 m. If the transverse jerk is struck at one end of the string, the disturbance will reach the other end in
(a) 1 second
(b) 0.5 second
(c) 2 seconds
(d) Data given is insufficient
Ans. (b)
Solution.
The speed of transverse wave in any string
μ = mass per unit length
Mass m = 2.5 kg
Hence wave speed
Time taken by the disturbance to travel from one end to the other end of the string i.e., to travel a distance of 20m is
Q.10. A train whistling at constant frequency is moving towards a station at a constant speed V. The train goes past a stationary observer on the station. The frequency n of the sound as heard by the observer is plotted as a function of time t (Figure) . Identify the expected curve.
(a)
(b)
(c)
(d)
Ans. (c)
Solution.
General expression for Apparent Frequency. Suppose observer (O) and source (S) are moving in the same direction along a line with velocities v0 and vs respectively. Velocity of sound is v and velocity of medium is vm, then apparent frequency observed by observer is given
If medium is stationary, i.e., vm = 0, then
Sign convention for different situations:
When train is approaching towards the observer.
Apparent frequency
It is clear that na > n0:
When the train is going away from the observer.
Apparent frequency
It is clear that na > no
Hence, the expected curve is (c).
MULTIPLE CHOICE QUESTIONS II
Q.11. A transverse harmonic wave on a string is described by y(x, t) = 3.0 sin (36t + 0.018x + π/4)
where x and y are in cm and t is in sec. The positive direction of x is from left to right.
(a) The wave is travelling from right to left.
(b) The speed of the wave is 20 m/s.
(c) Frequency of the wave is 5.7 Hz.
(d) The least distance between two successive crests in the wave is 2.5 cm.
Ans. (a,b,c)
Solution.
The general equation of a plane progressive wave with initial phase is
Various forms of progressive wave function:
Given equation is
y(x, t) = 3.0 sin (36 t + 0.018x + π/4)
Option (a): Since there is +ve sign between ωt and kx, the wave travels from right to left ( the positive direction of x is from left to right). Hence it is correct.
Option (b): Speed of the wave,
Hence it is correct.
Option (c): Frequency of the wave, Hence it is correct.
Option (d): Least distance between two successive crests,
Hence it is wrong.
Q.12. The displacement of a string is given by y(x, t) = 0.06 sin(2πx/3) cos(120πt) where x and y are in m and t in sec. The length of the string is 1.5 m and its mass is 3.0 x 10-2 kg.
(a) It represents a progressive wave of frequency 60 Hz.
(b) It represents a stationary wave of frequency 60 Hz.
(c) It is the result of superposition of two waves of wavelength 3 m, frequency 60 Hz each travelling with a speed of 180 m/s in opposite direction.
(d) Amplitude of this wave is constant.
Ans. (b, c)
Solution.
Standing Waves or Stationary Waves:
When two sets of progressive wave trains of same type (both longitudinal or both transverse) having the same amplitude and same time period/ frequency/wavelength travelling with same speed along the same straight line in opposite directions superimpose, a new set of waves are formed. These are called stationary waves or standing waves.
Suppose that the two superimposing waves are incident wave y1 = a sin(ωt - kx) and reflected wave y2 = a sin(ωt + kx).
(As y2 is the displacement due to a reflected wave from a free boundary).
Then by principle of superposition
y = y1 + y2 = a[sin(ωt - kx) + sin (ωt + kx)]
which gives the standard equation of stationary wave.
y(x, t) = 2a sin (kx) cos(ωt)
Given equation is
Option (a): Comparing with a standard equation of stationary wave y(x, t) = 2a sin (kx) cos(ωt)
Clearly, the given equation belongs to stationary wave. Hence, option (a) is not correct.
Option (b): By comparing, ω = 120π
⇒ 2πf = 120π
⇒ f = 60 Hz.
Hence it is correct.
Option (c):
⇒ λ = wavelength = 3 m
Frequency = f = 60 Hz
Speed = v = fλ = (60 Hz)(3 m) = 180 m/s. Hence it is correct.
Option(d): Since in stationary wave, all particles of the medium execute SHM with varying amplitude nodes. Hence, option (d) is not correct.
Q.13. Speed of sound waves in a fluid depends upon
(a) Directly on density of the medium.
(b) Square of Bulk modulus of the medium.
(c) Inversely on the square root of density.
(d) Directly on the square root of bulk modulus of the medium
Ans. (c, d)
Solution.
We define the speed of sound waves in a fluid as, Here B is the Bulk modulus and ρ is density of the medium.
It means, v ∝ 1/√ρ
[ ∴ for any fluid, B = constant]
and v ∝√B
[ ∵ for medium ρ = constant]
Hence, options (c) and (d) are correct.
Q.14. During propagation of a plane progressive mechanical wave
(a) All the particles are vibrating in the same phase.
(b) Amplitude of all the particles is equal.
(c) Particles of the medium executes S.H.M.
(d) Wave velocity depends upon the nature of the medium
Ans. (b, c, d)
Solution.
Characteristics of wave motion:
Option (a): Clearly, the particles 1, 2 and 3 are having different phase.
Option (b) and (c): Particles of the wave shown in the figure executes SHM with same amplitude.
Option (d): The wave velocity of mechanical wave depends only on elastic and inertia property of medium for a progressive wave propagating in a fluid. Hence wave velocity depends upon the nature of the medium.
Speed = v =
Hence, [ ∵ B is constant]
As ρ depends upon nature of the medium, hence v also depends upon the nature of the medium.
Q.15. The transverse displacement of a string (clamped at its both ends) is given by y (x,t) = 0.06 sin (2πx/3) cos (120πt).
All the points on the string between two consecutive nodes vibrate with
(a) Same frequency
(b) Same phase
(c) Same energy
(d) Different amplitude
Ans. (a, b, d)
Solution.
Q.16. A train, standing in a station yard, blows a whistle of frequency 400 Hz in still air. The wind starts blowing in the direction from the yard to the station with a speed of 10 m/s. Given that the speed of sound in still air is 340 m/s,
(a) The frequency of sound as heard by an observer standing on the platform is 400 Hz.
(b) The speed of sound for the observer standing on the platform is 350 m/s.
(c) The frequency of sound as heard by the observer standing on the platform will increase.
(d) The frequency of sound as heard by the observer standing on the platform will decrease.
Ans. (a, b)
Solution.
When the wind is blowing in the same direction as that of sound wave, then net speed of the wave is sum of speed of sound wave and speed of the wind.
Given, f0 = 400 Hz, v = 340 m/s Speed of wind vw = 10 m/s
Option (a): As there is no relative motion between the source and observer, hence frequency observed will be the same as natural frequency f0 = 400 Hz
Option (b): When the wind is blowing in the same direction as that of sound wave, then net speed of the wave is sum of speed of sound wave and speed of the wind. The speed of sound v = v + vw
= 340+ 10 = 350 m/s
Option (b) and (c): There will be no change in frequency because there is no relative motion between source and observer. Hence (c) and (d) are incorrect.
Q.17. Which of the following statements are true for a stationary wave?
(a) Every particle has a fixed amplitude which is different from the amplitude of its nearest particle.
(b) All the particles cross their mean position at the same time.
(c) All the particles are oscillating with same amplitude.
(d) There is no net transfer of energy across any plane.
(e) There are some particles which are always at rest.
Ans. (a, b, d, e)
Solution.
Consider the equation of a stationary wave
y(x, t) = 2a sin (kx) cos (wt)
Option (a): In stationary wave any particle at a given position have amplitude 2a sin kx.
Option (b): The time period of oscillation of all the particles is same, hence all the particles cross their mean position at the same time.
Option (c): Amplitude of all the particles are 2a sin kx which is different for different particles at different values of x.
Options (d) and (e): Nodes are the points which is always at rest hence no transfer of energy across the nodes. It means the energy is a stationary wave is confined between two nodes.
VERY SHORT ANSWER TYPE QUESTIONS
Q.1. A sonometer wire is vibrating in resonance with a tuning fork. Keeping the tension applied same, the length of the wire is doubled. Under what conditions would the tuning fork still be is resonance with the wire?
Ans. Wire of sonometer is twice the length which it vibrates in its second harmonic. Thus, if the tuning fork resonates at L, it will resonate at 2L. This can be explained as below:
The frequency of sonometer is given by
(n = number of loops)
For a given sonometer velocity of wave will be constant. If after changing the length of wire the tuning fork still be in resonance with the wire. Then, n/L = constant
Hence, when the wire is doubled the number of loops also get doubled to produce the resonance. That is it resonates in second harmonic.
Q.2. An organ pipe of length L open at both ends is found to vibrate in its first harmonic when sounded with a tuning fork of 480 Hz. What should be the length of a pipe closed at one end, so that it also vibrates in its first harmonic with the same tuning fork?
Ans. As, the medium and frequency and number of harmonic in open and closed pipes are same, so number of nodes and (wave), in both cases will be same.
In both end open pipe
and
In one end open pipe
As medium and turning fork in both cases are same v1 = v2 and c1 = c2 = c
or 4L2 = 2L1 or L2 = L1/2
So the length of one end closed pipe will be half of both end open pipe for resonant Ist harmonic with same frequency.
Q.3. A tuning fork A, marked 512 Hz, produces 5 beats per second, where sounded with another unmarked tuning fork B. If B is loaded with wax the number of beats is again 5 per second. What is the frequency of the tuning fork B when not loaded?
Ans. vA = 512, ∵ v0 = vA ∼ vB no. of frequency of beats
As on loading frequencies of B decreased
So in first case v1 = 5
When B is loads frequency of B is v
∴ i.e., vB either 507 or 517.
On load in frequency of B decreased 507 to lower value of number of beats will increase so vB ≠ 507. Now if vB = 517 then its frequency decrease by 10 Hz then number of beats will also be same as 512 – 507 = 5. So frequency of tuning fork when unloaded is 517.
Q.4. The displacement of an elastic wave is given by the function y = 3 sin ωt + 4 cos ωt. where y is in cm and t is in second. Calculate the resultant amplitude.
Ans. Given, displacement of the wave
y = 3 sin ωx + 4 cos ωx
Let us assume, 3 = A cos θ ...(i)
3 = Acos θ …(ii)
On dividing Eq. (ii) by Eq. (i)
tan θ = 4/3 => ϕ= tan-1(4/3)
Squaring and adding equations (i) and (ii),
A2 cos2 θ + A2 sin2 θ = 32 + 42
⇒ A2 (cos2 θ + sin2 θ) = 25
A2 = 25 ⇒ A = 5. Hence, amplitude = 5 cm
Frequency of vibrations,
Mass per unit length
∴
or f ∝ 1/r
Hence, when radius is tripled, the frequency will be 1/3 rd of previous value.
Q.5. A sitar wire is replaced by another wire of same length and material but of three times the earlier radius. If the tension in the wire remains the same, by what factor will the frequency change?
Ans. The wire is stretched both end so frequency of stretched wire is
As number of harmonic n, length L and tension (T) are kept same in both cases.
Mass per unit length
m = πr2ρ
As material of wire is same.
So the frequency of sitar reduced by 1/2 of previous value.
Q.6. At what temperatures (in oC) will the speed of sound in air be 3 times its value at 0oC?
Ans. We know that speed of sound in air
∴
But it is given,
⇒
∴ TT = 273 x 9 = 2457 K
= 2457 - 273 = 2184ºC
Q.7. When two waves of almost equal frequencies n1 and n2 reach at a point simultaneously, what is the time interval between successive maxima?
Ans. If two waves of almost equal frequencies interfere, they are producing beats.
Let n1 > n2
Beat frequency fbeat = n1 - n2
∴ Time period of beats
This time period will be equal to the time interval between successive maxima.
SHORT ANSWER TYPE QUESTIONS
Q.1. A steel wire has a length of 12 m and a mass of 2.10 kg. What will be the speed of a transverse wave on this wire when a tension of 2.06 × 104N is applied?
Ans. Given, length of the wire l = 12 m
Mass of wire m = 2.10 kg
Tension in wire T = 2.06 x 104 N
Speed of transverse wave v = where μ = Linear mass density = Mass per unit length, ⇒
Q.2. A pipe 20 cm long is closed at one end. Which harmonic mode of the pipe is resonantly excited by a source of 1237.5 Hz ?(sound velocity in air = 330 m s-1)
Ans. Length of pipe, l = 20 cm = 20 x 10-2 m
Fundamental frequency of closed organ pipe
It means third harmonic node of the pipe is resonantly excited by the source of given frequency.
Q.3. A train standing at the outer signal of a railway station blows a whistle of frequency 400 Hz still air. The train begins to move with a speed of 10 m s-1 towards the platform. What is the frequency of the sound for an observer standing on the platform? (sound velocity in air = 330 m s-1)
Ans. v0 = 400 Hz
vz = 10 m/s
Velocity of sound in air va = 330 m/s
Apparent frequency by observer standing on platform
Q.4. The wave pattern on a stretched string is shown in Figure Interpret what kind of wave this is and find its wavelength.
Ans. If we observe the graph there are some points on the graph which are always at rest. The points on positions x = 10,20,30,40 never move, always at mean position with respect to time. These are forming nodes which characterize a stationary wave.
We know the distance between two successive nodes is equal to λ/2
⇒ λ = 2 x (node to node distance)
= 2 x (20 - 10) = 20 cm
Q.5. The pattern of standing waves formed on a stretched string at two instants of time are shown in Figure. The velocity of two waves superimposing to form stationary waves is 360 ms-1 and their frequencies are 256 Hz.
(a) Calculate the time at which the second curve is plotted.
(b) Mark nodes and antinodes on the curve.
(c) Calculate the distance between A′ and C′ .
Ans. Given frequency of the wave v = 256 Hz
∴ T = 1/v = 1/256 second = 0.00390
T = 3.9 x 10-3 seconds.
(a) In stationary wave a particle passes through it’s mean position after ever T/4 time
∴ In IInd curve displacement of all medium particle, are zero so
(b) Point does not vibrate i.e., their displacement is zero always so nodes are at A, B, C, D and E. The point A’ and C’ are at maximum displacement so there are anti-nodes at A’ and C’.Between A and C =
Q.6. A tuning fork vibrating with a frequency of 512 Hz is kept close to the open end of a tube filled with water. The water level in the tube is gradually lowered. When the water level is 17 cm below the open end, maximum intensity of sound is heard. If the room temperature is 20° C, calculate
(a) speed of sound in air at room temperature
(b) speed of sound in air at 0° C
(c) if the water in the tube is replaced with mercury, will there be any difference in your observations?
Ans. If a pipe partially filled with water whose upper surface of the water acts as a reflecting surface of a closed organ pipe. If the length of the air column is varied until its natural frequency equals the frequency of the fork, then the column resonates and emits a loud note.
The frequency of tuning fork, f= 512 Hz.
For observation of first maxima of intensity,
The frequency of tuning fork, f = 512 Hz.
For observation of first maxima of intensity,
(a) For first maxima of intensity, the length of the air column Hence speed of sound v = fλ = 512 x (4 x 17 x 10-2)
= 348.16 m/s
(b) We know that v ∝ √T
where temperature (T) is in kelvin.
(c) The resonance will still be observed for 17 cm length of air column above mercury. However, due to more complete reflection of sound waves at mercury surface, the intensity of reflected sound increases.
Q.7. Show that when a string fixed at its two ends vibrates in 1 loop, 2 loops, 3 loops and 4 loops, the frequencies are in the ratio 1 : 2 : 3 : 4.
Ans. Let n be the number of loops in the string.
The length of each loop is λ/2
v = vλ and λ = u/v.So v = n/2L. (v) v is stretch string = For n = 1, If n = 2 then n = 3 then ∴ v1 : v2 : v3 : v4 = n1 : n2 : n3 : n4 = 1 : 2 : 3 : 4
LONG ANSWER TYPE QUESTIONS
Q.1. The earth has a radius of 6400 km. The inner core of 1000 km radius is solid. Outside it, there is a region from 1000 km to a radius of 3500 km which is in molten state. Then again from 3500 km to 6400 km the earth is solid. Only longitudinal (P) waves can travel inside a liquid. Assume that the P wave has a speed of 8 km s–1 in solid parts and of 5 km s–1 in liquid parts of the earth. An earthquake occurs at some place close to the surface of the earth. Calculate the time after which it will be recorded in a seismometer at a diametrically opposite point on the earth if wave travels along diameter?
Ans. r1 = 1000 km
r2 = 3500 km
r3 = 6400 km
d1 = 1000km
d2 = 3500 - 1000 =2500 km
d3 = 6400 - 3500 = 2900 km
Solid distance diametrically
= 2(d1 + d3) = 2(1000 +2900)
2 x 3900 km
Time taken by wave produced by earthquake in solid part
Liquid part along diametrically = 2d2 = 2 x 2500
∴ Time taken by seismic wave in liquid part Total time = 2[487.5 + 500] = 2 x 987.5 = 1975 sec.= 32 min 55 sec.
Q.2. If c is r.m.s. speed of molecules in a gas and v is the speed of sound waves in the gas, show that c/v is constant and independent of temperature for all diatomic gases.
Ans. We know that for molecules.M = molar mass of gas∵ PV = nRTn = 1
adiabatic constant for diatomic gasγ = 7/5
Q.3. Given below are some functions of x and t to represent the displacement of an elastic wave.
(a) y = 5 cos (4x ) sin(20t)
(b) y = 4 sin(5x – t/2) + 3 cos (5x – t/2)
(c) y = 10 cos [(252 – 250) πt ] cos [(252+250)πt ]
(d) y = 100 cos (100πt + 0.5x )
State which of these represent
(a) a travelling wave along –x direction
(b) a stationary wave
(c) beats
(d) a travelling wave along +x direction
Given reasons for your answers.
Ans. (a) A travelling wave along (-x) direction must have + kx i.e., in
(iv) V = 100 cos (100πt + 0.5x) so (a) (iv).
(b) A stationary wave of the for y = 5 cos (4x) sin 20t is a stationary wave so (b) (i).
(c) Beats involve (v1 + v2) and (v1 - v2) so beats can be represented by
y = 10 cos [ (252 - 250)πt] represents beat so (c) (iii).
(d) Let 4 = acosϕ ...(ii) and 3 = asinϕ ...(iii)a2 cos2ϕ + a2sin2ϕ= 42 + 32 squaring and adding (ii), (iii)
a2 = 25 K
⇒ a = 5
Substituting (ii), (iii) in (i)
Which represents the progressive wave in + x direction as the sign of kx (or 5x) and ωt(1/2 (t)) are opposite so it travels in + x direction. So (d) (ii)
Q.4. In the given progressive wave
y = 5 sin (100πt – 0.4πx )
where y and x are in m, t is in s. What is the
(a) amplitude
(b) wave length
(c) frequency
(d) wave velocity
(e) particle velocity amplitude
Ans. Standard form of progressive wave travelling in +x direction (kx and ωt have opposite sign is given)
Eqn. is y = a sin (ωt - kx + ϕ)
y = 5 sin(100πt - 0.4πx + 0)
(a) Amplitude a = 5m
(b) Wavelength λ, k = 2π/λ
k = 0.4π
(c) Frequency v, ω = 2 πv ⇒ v = ω/2π ∵ ω = 100π∴ (d) Wave velocity v = vλ = 50 x 5 = 250 m/s(e) Particle (medium) velocity in the direction of amplitude at a distance from source.
For maximum velocity of particle is at its mean positionvmax of medium particle = 500π m/s.
Q.5. For the harmonic travelling wave y = 2 cos 2π (10t–0.0080x + 3.5) where x and y are in cm and t is second. What is the phase difference between the oscillatory motion at two points separated by a distance of
(a) 4 m
(b) 0.5 m
(c) λ/2
(d) 3λ/4 (at a given instant of time)
(e) What is the phase difference between the oscillation of a particle located at x = 100cm, at t = T s and t = 5 s?
Ans. y = 2 cos 2π (10t - 0.0080 x + 3.5)
y = 2 cos (20πt - 0.016πx + 7.0π)
Wave is propagated in +x direction because ωt and kx are in with opposite sign standard equation y = acos (ωt - kx + ϕ)
a = 2, ω = 20π, k = 0.016π and ϕ = 7π
(a) path difference p = 4 m (given) = 400 cm
Phase difference Phase difference Δϕ = 6.4π rad.(b) Path difference p = 0.5 m = 50 cm
(c) Path difference p = λ/2x = 100 cmt = T
At x = 100, t = T
At t = 5sϕ2 = 20π(5) = 0.016π(100) + 7π = 100π - 1.6π + 7π = 105.4π
ϕ2 - ϕ1=105.4π - 7.4π = 98π radian
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