Simple Harmonic Motion

NEET Physics · 94 questions · Page 2 of 10 · Click an option or "Show Solution" to reveal answer

Q11
A body is executing simple harmonic motion with frequency 'n', the frequency of its potential energy is :
A 4n
B n
C 2n
D 3n
Correct Answer
Option C
Solution

Displacement equation of SHM of frequency 'n' x = A sin (ω\omegat) = A sin (2π\pint) Now, Potential energy

U=12kx2=12KA2sin2(2πnt)U = {1 \over 2}k{x^2} = {1 \over 2}K{A^2}{\sin ^2}(2\pi nt)
=12kA2[1cos(2π(2n)t)2]= {1 \over 2}k{A^2}\left[ {{{1 - \cos (2\pi (2n)t)} \over 2}} \right]

So frequency of potential energy = 2n

Q12
A spring is stretched by 5 cm by a force 10 N. The time period of the oscillations when a mass of 2 kg is suspended by it is -
A 0.628 s
B 0.0628 s
C 6.28 s
D 3.14 s
Correct Answer
Option A
Solution

F = Kx 10 = K ×\times 0.05 K =

10005=200{{1000} \over 5} = 200
T=2πmK=2π2200T = 2\pi \sqrt {{m \over K}} = 2\pi \sqrt {{2 \over {200}}}
=2π10=6.2810= {{2\pi } \over {10}} = {{6.28} \over {10}}

= .628 s

Q13
The phase difference between displacement and acceleration of a particle in a simple harmonic motion is :
A 3π2rad{{3\pi } \over 2}rad
B π2rad{\pi \over 2}rad
C zero
D π\pi rad
Correct Answer
Option D
Solution

Displacement, y = A.sin ω\omega t Velocity,

υ\upsilon

=

dydtAω.cosωt{{dy} \over {dt}}A\omega .\cos \omega t

Acceleration, a =

Aω2.sinωt- A{\omega ^2}.\sin \omega t
=Aω2.sin(ωt+π)= A{\omega ^2}.\sin \left( {\omega t + \pi } \right)

So the phase difference between y and a is π\pi.

Q14
The radius of circle, the period of revolution, initial position and sense of revolution are indicated is the figure. y- projection of the radius vector of rotating particle P is :
A y(t) = 4sin(πt2)\left( {{{\pi t} \over 2}} \right), where y in m
B y(t) = 3cos(3πt2)\left( {{{3\pi t} \over 2}} \right), where y in m
C y(t) = 3cos(πt2)\left( {{{\pi t} \over 2}} \right), where y in m
D y(t) = -3cos2π\pi t, where y in m
Correct Answer
Option C
Solution

Angular velocity, (ω\omega) =

2πT=2π4=π2{{2\pi } \over T} = {{2\pi } \over 4} = {\pi \over 2}

rad/s Since, at t = 0, displacement (y) is maximum, so equation will be cosine function. y = a cos ω\omegat \Rightarrow y = 3 cos

(πt2)\left( {{{\pi t} \over 2}} \right)
Q15
Average velocity of a particle executing SHM in one complete vibration is :
A Aω\omega
B Aω22{{A{\omega ^2}} \over 2}
C Aω2{{A\omega } \over 2}
D zero
Correct Answer
Option D
Solution

Since, net displacement in complete cycle ∆y = 0 So, Average velocity = Displacement Time travel =

yfyiT{{{y_f} - {y_i}} \over T}

=

ΔyT=0T=0{{\Delta y} \over T} = {0 \over T} = 0
Q16
The displacement of a particle executing simple harmonic motion is given by y = A 0 + A sinω\omega t + B cosω\omega t. Then the amplitude of its oscillation is given by :
A A2+B2\sqrt {{A^2} + {B^2}}
B A + B
C A + A2+B2\sqrt {{A^2} + {B^2}}
D A02+(A+B)2\sqrt {A_0^2 + {{\left( {A + B} \right)}^2}}
Correct Answer
Option A
Solution

From the given displacement y = A 0 + A sinω\omegat + B cosω\omegat.

Let assume, y - A 0 = γ\gamma γ\gamma = A sinω\omegat + B cosω\omegat =

A2+B2sin(ωt+ϕ)\sqrt {{A^2} + {B^2}} \sin \left( {\omega t + \phi } \right)

which is S.H.M \therefore Resultant amplitude of the particle, =

A2+B2\sqrt {{A^2} + {B^2}}
Q17
A pendulum is hung from the roof of a sufficiently high building and is moving freely to and fro like a simple harmonic oscillator. The acceleration of the bob of the pendulum is 20 m s –2 at a distance of 5 m from the mean position. The time period of oscillation is
A 2π\pi s
B π\pi s
C 2 s
D 1 s
Correct Answer
Option B
Solution

Given, acceleration, a = 20 m/s 2 , and displacement, y = 5m Magnitude of acceleration of a particle moving in a SHM is, |a| =

ω2{\omega ^2}

y; where y is amplitude. \Rightarrow 20 =

ω2{\omega ^2}

(5) \Rightarrow

ω=2\omega = 2

rad/s Time period of pendulum, T =

2πω=2π2{{2\pi } \over \omega } = {{2\pi } \over 2}

= π\pi s

Q18
A spring of force constant k is cut into lengths of ratio 1 : 2 : 3. They are connected in series and the new force constant is K'. Then they are connected in parallel and force constant is k''. Then k' : k'' is
A 1 : 9
B 1 : 11
C 1 : 14
D 1 : 6
Correct Answer
Option B
Solution

Let us assume, the length of spring be l.

When we cut the spring into ratio of length 1 : 2 : 3, we get three springs of lengths

l6,2l6{l \over 6},{{2l} \over 6}

and

3l6{{3l} \over 6}

with force constant, \therefore

k1=kll1=kll/6=6k{k_1} = {{kl} \over {{l_1}}} = {{kl} \over {l/6}} = 6k
k2=kll2=kl2l/6=3k{k_2} = {{kl} \over {{l_2}}} = {{kl} \over {2l/6}} = 3k
k3=kll3=kl3l/6=2k{k_3} = {{kl} \over {{l_3}}} = {{kl} \over {3l/6}} = 2k

When connected in series,

1k=16k+13k+12k=1+2+36k=1k{1 \over {k'}} = {1 \over {6k}} + {1 \over {3k}} + {1 \over {2k}} = {{1 + 2 + 3} \over {6k}} = {1 \over k}
k=k\therefore k' = k

When connected in parallel, k'' = 6k + 3k + 2k = 11k

kk=k11k=111{{k'} \over {k''}} = {k \over {11k}} = {1 \over {11}}
Q19
A particle executes linear simple harmonic motion with an amplitude of 3 cm. When the particle is at 2 cm from the mean position, the magnitude of its velocity is equal to that of its acceleration. Then its time period in second is
A 52π{{\sqrt 5 } \over {2\pi }}
B 4π5{{4\pi } \over {\sqrt 5 }}
C 2π3{{2\pi } \over {\sqrt 3 }}
D 5π{{\sqrt 5 } \over \pi }
Correct Answer
Option B
Solution

Given, Amplitude A = 3 cm When particle is at x = 2 cm According to question, magnitude of velocity = acceleration

ωA2x2=xω2\omega \sqrt {{A^2} - {x^2}} = x{\omega ^2}
(3)2(2)2=2(2πT)\sqrt {{{\left( 3 \right)}^2} - {{\left( 2 \right)}^2}} = 2\left( {{{2\pi } \over T}} \right)
5=4πTT=4π5\sqrt 5 = {{4\pi } \over T} \Rightarrow T = {{4\pi } \over {\sqrt 5 }}
Q20
A body of mass m is attached to the lower end of a spring whose upper end is fixed. The spring has negligible mass. When the mass m is slightly pulled down and released, it oscillates with a time period of 3s. When the mass m is increased by 1 kg, the time period of oscillations becomes 5 s. The value of m in kg is
A 34{3 \over 4}
B 43{4 \over 3}
C 169{{16} \over 9}
D 916{9 \over {16}}
Correct Answer
Option D
Solution

The time period of oscillation is given by

T=2πm/kT = 2\pi \sqrt {m/k}
T1=3=2πm/k{T_1} = 3 = 2\pi \sqrt {m/k}
T2=5=2π(m+1k){T_2} = 5 = 2\pi \sqrt {\left( {{{m + 1} \over k}} \right)}

On dividing :

3/5=m/(m+1)3/5 = \sqrt {m/\left( {m + 1} \right)}
9/25=m/(m+1)9/25 = \sqrt {m/\left( {m + 1} \right)}
9m+9=25m9m + 9 = 25m
16m=9m=9/1616m = 9 \Rightarrow m = 9/16
Ready for a full NEET mock test? Timed · full syllabus · instant results
Take a Mock Test →