Waves

JEE Physics · 96 questions · Page 7 of 10 · Click an option or "Show Solution" to reveal answer

Q61
The fundamental frequency of a closed organ pipe is equal to the first overtone frequency of an open organ pipe. If length of the open pipe is 60 cm60 \mathrm{~cm}, the length of the closed pipe will be:
A 15 cm
B 60 cm
C 45 cm
D 30 cm
Correct Answer
Option A
Solution
f1=v4 L1f1=f2v4 L1=vL2L2=4 L160=4×L1 L1=15 cm\begin{aligned} & \mathrm{f}_1=\frac{\mathrm{v}}{4 \mathrm{~L}_1} \\ & \mathrm{f}_1=\mathrm{f}_2 \\ & \frac{\mathrm{v}}{4 \mathrm{~L}_1}=\frac{\mathrm{v}}{\mathrm{L}_2} \\ & \Rightarrow \mathrm{L}_2=4 \mathrm{~L}_1 \\ & 60=4 \times \mathrm{L}_1 \\ & \mathrm{~L}_1=15 \mathrm{~cm} \end{aligned}
Q62
A plane progressive wave is given by y=2cos2π(330tx)my=2 \cos 2 \pi(330 \mathrm{t}-x) \mathrm{m}. The frequency of the wave is :
A 660 Hz
B 340 Hz
C 330 Hz
D 165 Hz
Correct Answer
Option C
Solution

To find the frequency of the plane progressive wave given by the equation

y=2cos2π(330tx)my = 2 \cos 2 \pi(330 \mathrm{t} - x) \mathrm{m}

, we start by analyzing the general form of a wave equation. The general form of a wave equation is:

y=Acos(2πftkx+ϕ)y = A \cos (2 \pi ft - kx + \phi)

where:

AA

is the amplitude of the wave.

ff

is the frequency of the wave.

tt

is the time variable.

kk

is the wave number, defined as

2πλ\frac{2 \pi}{\lambda}

where λ\lambda is the wavelength.

xx

is the spatial variable. ϕ\phi is the phase constant.

By comparing the given wave equation with the general form, we have:

y=2cos2π(330tx)y = 2 \cos 2 \pi (330 t - x)

We observe that the term

2π(330tx)2 \pi(330t - x)

corresponds to

2πftkx2 \pi ft - kx

in the general form. From this, it is clear that:

2πft2π330t2 \pi ft \rightarrow 2 \pi \cdot 330 t

Therefore,

f=330f = 330

Hz So, the frequency of the wave is 330 Hz. Thus, the correct answer is: Option C: 330 Hz

Q63
A closed organ and an open organ tube are filled by two different gases having same bulk modulus but different densities ρ1\rho_1 and ρ2\rho_2, respectively. The frequency of 9th 9^{\text{th }} harmonic of closed tube is identical with 4th 4^{\text{th }} harmonic of open tube. If the length of the closed tube is 10 cm and the density ratio of the gases is ρ1:ρ2=1:16\rho_1: \rho_2=1: 16, then the length of the open tube is :
A 157 cm\dfrac{15}{7} \mathrm{~cm}
B 209 cm\dfrac{20}{9} \mathrm{~cm}
C 207 cm\dfrac{20}{7} \mathrm{~cm}
D 159 cm\dfrac{15}{9} \mathrm{~cm}
Correct Answer
Option B
Solution

We know, for closed pipe,

fn=nv4l,n=1,3,5,7{f_n} = {{nv} \over {4l}},\,n = 1,3,5,7

for open pipe,

fn=nv2L,n=1,2,3,4{f_n} = {{nv} \over {2L}},\,n = 1,2,3,4

So, 9th^{th} harmonic of closed pipe

=9v14l1= {{9{v_1}} \over {4{l_1}}}

4th^{th} harmonic of open pipe

=4v22l2=2v2l2= {{4{v_2}} \over {2{l_2}}} = {{2{v_2}} \over {{l_2}}}

\therefore

9v14l1=2v2l2l2l1=89v2v1{{9{v_1}} \over {4{l_1}}} = {{2{v_2}} \over {{l_2}}} \Rightarrow {{{l_2}} \over {{l_1}}} = {8 \over 9}{{{v_2}} \over {{v_1}}}

We know,

v=βρv = \sqrt {{\beta \over \rho }}

So,

v2v1=ρ1ρ2{{{v_2}} \over {{v_1}}} = \sqrt {{{{\rho _1}} \over {{\rho _2}}}}

(for same β\beta) hence,

l2l1=89ρ1ρ2=89116=89×14{{{l_2}} \over {{l_1}}} = {8 \over 9}\sqrt {{{{\rho _1}} \over {{\rho _2}}}} = {8 \over 9}\sqrt {{1 \over {16}}} = {8 \over 9} \times {1 \over 4}
l2=29×l1l2=29×10=209cm\Rightarrow {l_2} = {2 \over 9} \times {l_1} \Rightarrow {l_2} = {2 \over 9} \times 10 = {{20} \over 9}cm
Q64
The amplitude and phase of a wave that is formed by the superposition of two harmonic travelling waves, y1(x,t)=4sin(kxωt)y_1(x, t) = 4 \sin (kx - \omega t) and y2(x,t)=2sin(kxωt+2π3)y_2(x, t) = 2 \sin (kx - \omega t + \dfrac{2\pi}{3}), are: (Take the angular frequency of initial waves same as ω\omega)
A [3,π6]\left[\sqrt{3}, \dfrac{\pi}{6}\right]
B [23,π6]\left[2\sqrt{3}, \dfrac{\pi}{6}\right]
C [6,2π3]\left[6, \dfrac{2\pi}{3}\right]
D [6,π3]\left[6, \dfrac{\pi}{3}\right]
Correct Answer
Option B
Solution

To determine the amplitude and phase of the wave formed by the superposition of the two harmonic traveling waves, y1(x,t)=4sin(kxωt) y_1(x, t) = 4 \sin (kx - \omega t) and y2(x,t)=2sin(kxωt+2π3) y_2(x, t) = 2 \sin (kx - \omega t + \dfrac{2\pi}{3}) , we use the following steps: First, calculate the resultant amplitude A A using the formula for the resultant of two waves with different phases: A=A12+A22+2A1A2cos(ϕ) A = \sqrt{A_1^2 + A_2^2 + 2 A_1 A_2 \cos(\phi)} where: A1=4 A_1 = 4 (amplitude of the first wave) A2=2 A_2 = 2 (amplitude of the second wave) ϕ=120 \phi = 120^\circ (phase difference, given by 2π3\dfrac{2\pi}{3}).

Substituting the values, we get: A=42+22+2×4×2×cos(120) A = \sqrt{4^2 + 2^2 + 2 \times 4 \times 2 \times \cos(120^\circ)} cos(120)=12 \cos(120^\circ) = -\dfrac{1}{2} Therefore: A=16+4+16×(12) A = \sqrt{16 + 4 + 16 \times (-\dfrac{1}{2})} A=16+48 A = \sqrt{16 + 4 - 8} A=12=23 A = \sqrt{12} = 2\sqrt{3} Next, compute the phase ϕ \phi of the resultant wave: tanϕ=A2sin(ϕ)A1+A2cos(ϕ) \tan \phi = \dfrac{A_2 \sin(\phi)}{A_1 + A_2 \cos(\phi)} tanϕ=2sin(120)4+2cos(120) \tan \phi = \dfrac{2 \sin(120^\circ)}{4 + 2 \cos(120^\circ)} sin(120)=32andcos(120)=12 \sin(120^\circ) = \dfrac{\sqrt{3}}{2} \quad \text{and} \quad \cos(120^\circ) = -\dfrac{1}{2} Substituting these values, we get: tanϕ=2×324+2×12 \tan \phi = \dfrac{2 \times \dfrac{\sqrt{3}}{2}}{4 + 2 \times -\dfrac{1}{2}} tanϕ=33 \tan \phi = \dfrac{\sqrt{3}}{3} This simplifies to: ϕ=π6 \phi = \dfrac{\pi}{6} Thus, the amplitude and phase of the resultant wave are 23 2\sqrt{3} and π6 \dfrac{\pi}{6} respectively.

Q65
A sinusoidal wave of wavelength 7.5 cm travels a distance of 1.2 cm along the xx-direction in 0.3 sec . The crest P is at x=0x=0 at t=0sec\mathrm{t}=0 \mathrm{sec} and maximum displacement of the wave is 2 cm . Which equation correctly represents this wave?
A y=2cos(0.83x3.35t)cmy=2 \cos (0.83 x-3.35 t) \mathrm{cm}
B y=2sin(0.83x3.5t)cmy=2 \sin (0.83 x-3.5 \mathrm{t}) \mathrm{cm}
C y=2cos(0.13x0.5t)cmy=2 \cos (0.13 x-0.5 t) \mathrm{cm}
D y=2cos(3.35x0.83t)cmy=2 \cos (3.35 x-0.83 \mathrm{t}) \mathrm{cm}
Correct Answer
Option A
Solution

To find the equation of the sinusoidal wave, we need to determine several properties of the wave: Wave Velocity (v): Given that the wave travels a distance of 1.2 cm in 0.3 seconds, the velocity v v can be computed as: v=distancetime=1.2cm0.3s=4cm/s v = \dfrac{\text{distance}}{\text{time}} = \dfrac{1.2 \, \text{cm}}{0.3 \, \text{s}} = 4 \, \text{cm/s} Wave Number (k): The wave number k k is calculated using the wavelength λ=7.5cm \lambda = 7.5 \, \text{cm} : k=2πλ=2π7.5=4π150.83 k = \dfrac{2\pi}{\lambda} = \dfrac{2\pi}{7.5} = \dfrac{4\pi}{15} \approx 0.83 Angular Frequency (ω\omega): Angular frequency ω \omega is related to the wave number and velocity by the equation v=ωk v = \dfrac{\omega}{k} , thus: ω=vk=4×4π15=16π153.35 \omega = vk = 4 \times \dfrac{4\pi}{15} = \dfrac{16\pi}{15} \approx 3.35 Wave Equation: The general form for a sinusoidal wave traveling in the positive x-direction is: y=Acos(kxωt) y = A \cos(kx - \omega t) Given the maximum displacement (amplitude A A ) of the wave is 2 cm, the equation becomes: y=2cos(0.83x3.35t)cm y = 2 \cos(0.83x - 3.35t) \, \text{cm} This equation accurately describes the sinusoidal wave given the provided parameters.

Q66
In an experiment with a closed organ pipe, it is filled with water by (15)\left(\dfrac{1}{5}\right) th of its volume. The frequency of the fundamental note will change by
A 20%20 \%
B 25%25 \%
C 20%-20 \%
D 25%-25 \%
Correct Answer
Option B
Solution
λ1=4f1=v4\begin{aligned} &\lambda_1=4 \ell\\ &\mathrm{f}_1=\frac{\mathrm{v}}{4 \ell} \end{aligned}
λ2=165f2=5 V16Δff=V(116)V4×100=25%\begin{aligned} & \lambda_2=\frac{16 \ell}{5} \\ & \mathrm{f}_2=\frac{5 \mathrm{~V}}{16 \ell} \\ & \frac{\Delta \mathrm{f}}{\mathrm{f}}=\frac{\frac{\mathrm{V}}{\ell}\left(\frac{1}{16}\right)}{\frac{\mathrm{V}}{4 \ell}} \times 100=25 \% \end{aligned}
Q67
A wave travelling along the xx-axis is described by the equation y(x,t)=0.005y(x, t)=0.005 cos(αxβt).\cos \,\left( {\alpha \,x - \beta t} \right). If the wavelength and the time period of the wave are 0.080.08 mm and 2.0s2.0s, respectively, then α\alpha and β\beta in appropriate units are
A α=25.00π,β=π\alpha = 25.00\pi ,\,\beta = \pi
B α=0.08π,β=2.0π\alpha = {{0.08} \over \pi },\,\beta = {{2.0} \over \pi }
C α=0.04π,β=1.0π\alpha = {{0.04} \over \pi },\,\beta = {{1.0} \over \pi }
D α=12.50π,β=π2.0\alpha = 12.50\pi ,\,\beta = {\pi \over {2.0}}
Correct Answer
Option A
Solution
y(x,t)=0.005cos(αxβt)y\left( {x,t} \right) = 0.005\,\cos \left( {\alpha x - \beta t} \right)

(Given) Comparing it with the standard equation of wave

y(x,t)=acos(kxωt)y\left( {x,t} \right) = a\cos \left( {kx - \omega t} \right)

we get

k=αk = \alpha
\,\,\,\,\,

and

\,\,\,\,\,
ω=β\omega = \beta

\therefore

2πγ=α{{2\pi } \over \gamma } = \alpha
\,\,\,\,\,

and

\,\,\,\,\,
2πT=β{{2\pi } \over T} = \beta

\therefore

α=2π0.08=25π\alpha = {{2\pi } \over {0.08}} = 25\pi
\,\,\,\,\,

and

\,\,\,\,\,
β=2π2=π\beta = {{2\pi } \over 2} = \pi
Q68
The equation of a wave travelling on a string is y = sin[20πx + 10πt], where x and t are distance and time in SI units. The minimum distance between two points having the same oscillating speed is :
A 10 cm
B 2.5 cm
C 20 cm
D 5.0 cm
Correct Answer
Option D
Solution

The equation for a wave traveling on a string is given by y=sin(20πx+10πt) y = \sin(20\pi x + 10\pi t) , where x x is the distance and t t is the time in SI units.

To find the minimum distance between two points having the same oscillating speed, we use the concept that this distance is half the wavelength (λ2)\left(\dfrac{\lambda}{2}\right).

To find the wavelength λ\lambda: λ=2πk \lambda = \dfrac{2\pi}{k} Here, the wave number k=20π k = 20\pi .

Thus, λ=2π20π=110 m=10 cm \lambda = \dfrac{2\pi}{20\pi} = \dfrac{1}{10} \text{ m} = 10 \text{ cm} Thus, the minimum distance between two points having the same speed is: Distance=λ2=10 cm2=5 cm \text{Distance} = \dfrac{\lambda}{2} = \dfrac{10 \text{ cm}}{2} = 5 \text{ cm}

Q69
A heavy ball of mass M is suspendeed from the ceiling of a car by a light string of mass m (m < < M). When the car is at rest, the speed of transverse waves in the string is 60 ms-1. When the car has acceleration a, the wave-speed increases to 60.5 ms-1. The value of a, in terms of gravitational acceleration g, is closest to :
A g30{g \over {30}}
B g5{g \over 5}
C g10{g \over 10}
D g20{g \over 20}
Correct Answer
Option B
Solution

Resultant force on the ball of mass M when car is moving with a acceleration a is , Fnet =

(Mg)2+(Ma)2\sqrt {{{\left( {Mg} \right)}^2} + {{\left( {Ma} \right)}^2}}

=

Mg2+a2M\sqrt {{g^2} + {a^2}}

\therefore T = M

g2+a2\sqrt {{g^2} + {a^2}}

We know, Velocity, V =

Tμ\sqrt {{T \over \mu }}

When Car is at rest then, 60 =

Mgμ\sqrt {{{Mg} \over \mu }}

. . . . (1) and when is moving then 60.5 =

Mg2+a2μ\sqrt {{{M\sqrt {{g^2} + {a^2}} } \over \mu }}

. . . . (2) By dividing (2) by (1) we get,

60.560=g2+a2g{{60.5} \over {60}} = \sqrt {{{\sqrt {{g^2} + {a^2}} } \over g}}

\Rightarrow

(1+0.560)\left( {1 + {{0.5} \over {60}}} \right)

=

(g2+a2g2)14{\left( {{{{g^2} + {a^2}} \over {{g^2}}}} \right)^{{1 \over 4}}}

\Rightarrow

g2+a2g2{{{g^2} + {a^2}} \over {{g^2}}}

=

(1+0.560)4{\left( {1 + {{0.5} \over {60}}} \right)^4}

\Rightarrow

g2+a2g2{{{g^2} + {a^2}} \over {{g^2}}}

= 1 + 4 ×\times

0.560{{{0.5} \over {60}}}

[Using Binomial approximation] \Rightarrow

g2+a2g2{{{g^2} + {a^2}} \over {{g^2}}}

= 1 +

130{1 \over {30}}

\Rightarrow 1 +

a2g2{{{a^2}} \over {{g^2}}}

= 1 +

130{1 \over {30}}

\Rightarrow

ag{a \over g}

=

130{1 \over {\sqrt {30} }}

\Rightarrow a =

g30{g \over {\sqrt {30} }}

\therefore Closest answer, a =

g5{g \over 5}
Q70
A tuning fork A of unknown frequency produces 5 beats/s with a fork of known frequency 340 Hz. When fork A is filed, the beat frequency decreases to 2 beats/s. What is the frequency of fork A?
A 335 Hz
B 345 Hz
C 338 Hz
D 342 Hz
Correct Answer
Option A
Solution

Initially beat frequency = 5Hz so, ρ\rhoA = 340 ±\pm 5 = 345 Hz, or 335 Hz after filing frequency increases slightly so, new value of frequency of A > ρ\rhoA Now, beat frequency = 2Hz \Rightarrow new ρ\rhoA = 340 ±\pm 2 = 342 Hz, or 338 Hz hence, original frequency of A is ρ\rhoA = 335 Hz

Ready for a full JEE mock test? Timed · full syllabus · instant results
Take a Mock Test →