Simple Harmonic Motion

NEET Physics · 94 questions · Page 6 of 10 · Click an option or "Show Solution" to reveal answer

Q51
Two particles A and B of equal masses are suspended from two massless springs of spring constants K1 and K2 respectively. If the maximum velocities during oscillations are equal, the ratio of the amplitude of A and B is
A K1K2{{{K_1}} \over {{K_2}}}
B K1K2\sqrt {{{{K_1}} \over {{K_2}}}}
C K2K1{{{K_2}} \over {{K_1}}}
D K2K1\sqrt {{{{K_2}} \over {{K_1}}}}
Correct Answer
Option D
Solution

\because

Vmax=Aω{V_{\max }} = A\omega

Given,

ω1A1=ω2A2{\omega _1}{A_1} = {\omega _2}{A_2}

We know that

ω=Km\omega = \sqrt {{K \over m}}

\therefore

k1mA1=k2mA2\sqrt {{{{k_1}} \over m}} {A_1} = \sqrt {{{{k_2}} \over m}} {A_2}

\Rightarrow

A1A2=k2k1{{{A_1}} \over {{A_2}}} = \sqrt {{{{k_2}} \over {{k_1}}}}
Q52
Starting from the origin a body oscillates simple harmonically with a period of 22 s.s. After what time will its kinetic energy be 75%75\% of the total energy?
A 16s{1 \over 6}s
B 14s{1 \over 4}s
C 13s{1 \over 3}s
D 112s{1 \over 12}s
Correct Answer
Option A
Solution
K.E.K.E.\,

of a body undergoing

SHMSHM

is given by,

K.E.=12ma2ω2cos2ωt,K.E. = {1 \over 2}m{a^2}{\omega ^2}{\cos ^2}\,\omega t,
T.E.=12ma2ω2T.E. = {1 \over 2}m{a^2}{\omega ^2}

Given

K.E.=0.75T.E.K.E.=0.75T.E.
0.75=cos2ωtωt=π6\Rightarrow 0.75 = {\cos ^2}\omega t \Rightarrow \omega t = {\pi \over 6}
t=π6×ωt=π×26×2πt=16s\Rightarrow t = {\pi \over {6 \times \omega }} \Rightarrow t = {{\pi \times 2} \over {6 \times 2\pi }} \Rightarrow t = {1 \over 6}s
Q53
The displacement of simple harmonic oscillator after 3 seconds starting from its mean position is equal to half of its amplitude. The time period of harmonic motion is :
A 6 s
B 8 s
C 12 s
D 36 s
Correct Answer
Option D
Solution

Time taken by the harmonic oscillator to move from mean position to half of amplitude is

T12{T \over {12}}

So,

T12{T \over {12}}

= 3 T = 36 sec.

Q54
A simple pendulum doing small oscillations at a place RR height above earth surface has time period of T1=4 sT_1=4 \mathrm{~s}. T2\mathrm{T}_2 would be it's time period if it is brought to a point which is at a height 2R2 \mathrm{R} from earth surface. Choose the correct relation [R=\mathrm{R}= radius of earth] :
A 3 T1=2 T23 \mathrm{~T}_1=2 \mathrm{~T}_2
B T1=T2\mathrm{T}_1=\mathrm{T}_2
C 2 T1=3 T22 \mathrm{~T}_1=3 \mathrm{~T}_2
D 2 T1=T22 \mathrm{~T}_1=\mathrm{T}_2
Correct Answer
Option A
Solution

The time period of a simple pendulum is given by the formula:

T=2πlgT = 2\pi \sqrt{\frac{l}{g}}

where

TT

is the time period,

ll

is the length of the pendulum, and

gg

is the acceleration due to gravity at the location of the pendulum.

The acceleration due to gravity changes with height above the Earth's surface.

The acceleration due to gravity at a height

hh

above the Earth's surface can be expressed as:

g=g(RR+h)2g' = g \left(\frac{R}{R + h}\right)^2

where

gg

is the acceleration due to gravity at the surface of the Earth,

RR

is the radius of the Earth, and

hh

is the height above the Earth’s surface.

Since the time period of the pendulum depends on the square root of the inverse of the acceleration due to gravity, any change in

gg

due to a change in height will affect the time period. Given that the time period of the pendulum at a height

RR

above Earth's surface is

T1T_1

, and we're to find the time period

T2T_2

at a height of

2R2R

, we can use the formula for acceleration due to gravity at different heights to express the relationship between

T1T_1

and

T2T_2

. For the initial case at height

RR

:

g1=g(RR+R)2=g(R2R)2=g4g_1 = g \left(\frac{R}{R + R}\right)^2 = g \left(\frac{R}{2R}\right)^2 = \frac{g}{4}

For the new case at height

2R2R

:

g2=g(RR+2R)2=g(R3R)2=g9g_2 = g \left(\frac{R}{R + 2R}\right)^2 = g \left(\frac{R}{3R}\right)^2 = \frac{g}{9}

The time period is proportional to the square root of the inverse of

gg

, so:

T1T2=g2g1=g9g4=49=23\frac{T_1}{T_2} = \sqrt{\frac{g_2}{g_1}} = \sqrt{\frac{\frac{g}{9}}{\frac{g}{4}}} = \sqrt{\frac{4}{9}} = \frac{2}{3}

Therefore:

T1=23T2T_1 = \frac{2}{3}T_2

Rearranging this equation:

3T1=2T23T_1 = 2T_2

This corresponds to Option A.

Q55
The maximum velocity of a particle, executing simple harmonic motion with an amplitude 77 mm,mm, is 4.44.4 m/s.m/s. The period of oscillation is
A 0.010.01 ss
B 1010 ss
C 0.10.1 ss
D 100100 ss
Correct Answer
Option A
Solution

Maximum velocity,

vmax=aω,vmax=a×2πT{v_{\max }} = a\omega ,\,\,\,\,\,{v_{\max }} = a \times {{2\pi } \over T}
T=2πavmax=2×3.14×7×1034.40.01s\Rightarrow T = {{2\pi a} \over {{v_{\max }}}} = {{2 \times 3.14 \times 7 \times {{10}^{ - 3}}} \over {4.4}} \approx 0.01\,s
Q56
Two particles are performing simple harmonic motion in a straight line about the same equilibrium point. The amplitude and time period for both particles are same and equal to A and I, respectively. At time t = 0 one particle has displacement A while the other one has displacement A2{{ - A} \over 2} and they are moving towards each other. If they cross each other at time t, then t is :
A T6{T \over 6}
B 5T6{5T \over 6}
C T3{T \over 3}
D T4{T \over 4}
Correct Answer
Option A
Solution

Angular displacement (θ\theta1) of particle 1. from equilibrium,

y1{y_1}

= A sinθ\theta1 \Rightarrow A = Asinθ\theta1 \Rightarrow sinθ\theta1 = 1 = sin

π2{\pi \over 2}

\therefore θ\theta1 =

π2{\pi \over 2}

Similarly for particle 2 angular displacement θ\theta2 from equilibrium, y2 = Asinθ\theta2 \Rightarrow -

A2{A \over 2}

= Asinθ\theta2 \Rightarrow sinθ\theta2 = -

12{1 \over 2}

= sin

(π3)\left( { - {\pi \over 3}} \right)

\Rightarrow θ\theta2 = -

π3{{\pi \over 3}}

Relative angular displacement of the two particle, θ\theta = θ\theta1 - θ\theta2 =

π2{{\pi \over 2}}

-

(π6)\left( { - {\pi \over 6}} \right)

=

2π3{{{2\pi } \over 3}}

Relative angular velocity ==

ω(ω)\omega - \left( { - \omega } \right)

=

2ω2\omega

If they cross each other at time t then, t =

θ2ω{\theta \over {2\omega }}

=

2π3×2ω{{2\pi } \over {3 \times 2\omega }}

=

π3×2πT{\pi \over {3 \times {{2\pi } \over T}}}

=

T6{T \over 6}
Q57
A particle executes simple harmonic motion between x=Ax=-A and x=+Ax=+A. If time taken by particle to go from x=0x=0 to A2\dfrac{A}{2} is 2 s; then time taken by particle in going from x=A2x=\dfrac{A}{2} to A is
A 4 s
B 1.5 s
C 3 s
D 2 s
Correct Answer
Option A
Solution

x=Asin(ωt)x=A \sin (\omega t)

x=A2=Asin(ωt)12=sin(ωt)t=(π6ω)=2πω=12sec\begin{aligned} & x=\frac{A}{2}=A \sin (\omega t) \\\\ & \frac{1}{2}=\sin (\omega t) \\\\ & t=\left(\frac{\pi}{6 \omega}\right)=2 \\\\ & \frac{\pi}{\omega}=12 \sec \end{aligned}

x=A=Asin(ωt)x=A=A \sin (\omega t) ωt=(π2)\omega t=\left(\dfrac{\pi}{2}\right) t=(π2ω)=6t=\left(\dfrac{\pi}{2 \omega}\right)=6 second time =62=4=6-2=4 seconds

Q58
Given below are two statements : Statement I : A second's pendulum has a time period of 1 second. Statement II : It takes precisely one second to move between the two extreme positions. In the light of the above statements, choose the correct answer from the options given below :
A Both Statement I and Statement II are false
B Statement I is false but Statement II is true
C Both Statement I and Statement II are true
D Statement I is true but Statement II is false
Correct Answer
Option B
Solution

As we know time period of second’s penduklum is 2 sec, so statement (1) is incorrect.

Time taken by particle performing SHM between two extreme position is half of the time period.

Here, T = 2 sec.

So, time = 2/2 = 1 sec

Q59
Two simple pendulums having lengths l1l_1 and l2l_2 with negligible string mass undergo angular displacements θ1\theta_1 and θ2\theta_2, from their mean positions, respectively. If the angular accelerations of both pendulums are same, then which expression is correct?
A θ1l2=θ2l1\theta_1 l_2=\theta_2 l_1
B θ1l1=θ2l2\theta_1 l_1=\theta_2 l_2
C θ1l22=θ2l12\theta_1 l_2^2=\theta_2 l_1^2
D θ1l12=θ2l22\theta_1 l_1^2=\theta_2 l_2^2
Correct Answer
Option A
Solution

Angular Frequency: The angular frequency (ω\omega) of a simple pendulum is given by: ω=g \omega = \sqrt{\dfrac{g}{\ell}} where gg is the acceleration due to gravity and \ell is the pendulum length.

Angular Acceleration: The angular acceleration (α\alpha) can be expressed in terms of angular displacement (θ\theta) and angular frequency: α=ω2θ \alpha = -\omega^2 \theta Equating Angular Accelerations: Since the angular accelerations of the two pendulums are equal, we equate them: g1θ1=g2θ2 \dfrac{g}{\ell_1} \theta_1 = \dfrac{g}{\ell_2} \theta_2 Simplifying the Expression: By canceling out gg on both sides, we derive: θ12=θ21 \theta_1 \ell_2 = \theta_2 \ell_1 Thus, the correct expression that relates the displacements and lengths of the pendulums is θ12=θ21\theta_1 \ell_2 = \theta_2 \ell_1.

Q60
A child swinging on a swing in sitting position, stands up, then the time period of the swing will
A increase
B decrease
C remains same
D increases of the child is long and decreases if the child is short
Correct Answer
Option B
Solution

KEY CONCEPT : The time period

T=2πgT = 2\pi \sqrt {{\ell \over g}}

where

\ell

== distance between the point of suspension and the center of mass of the child.

This distance decreases when the child stands \therefore

T<TT' < T

i.e., the period decreases.

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