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Question: A particle is describing simple harmonic motion. If its velocities are \[{v_1}\]​ and \[{v_2}\]when ...

A particle is describing simple harmonic motion. If its velocities are v1{v_1}​ and v2{v_2}when the displacements from the mean position are y1{y_1}and y2{y_2}respectively, then its time period is
a. 2πy12+y22v12+v222\pi \sqrt {\dfrac{{y_1^2 + y_2^2}}{{v_1^2 + v_2^2}}}
b. 2πv22v12y12y222\pi \sqrt {\dfrac{{v_2^2 - v_1^2}}{{y_1^2 - y_2^2}}}
c. 2πv22+v12y12+y222\pi \sqrt {\dfrac{{v_2^2 + v_1^2}}{{y_1^2 + y_2^2}}}
d. 2πy12y22v22v122\pi \sqrt {\dfrac{{y_1^2 - y_2^2}}{{v_2^2 - v_1^2}}}

Explanation

Solution

We can write Simple harmonic motion as SHM. SHM is known as a special type of periodic motion. In question the time period of a particle is calculated. The period is defined by the time it takes for one oscillation. In question, we are using the phenomenon of SHM to calculate the time period of moving particles.

Formula used:
Simple harmonic motion is also known as a periodic oscillation. we can measure its period. To calculate time period, first we find from, velocity formula v=ωA2y2v = \omega \sqrt {{A^2} - {y^2}} .v1{v_1} and v2{v_2}can be calculated by putting and on above formula. Then using angular frequency formulaω=2πT\omega = \dfrac{{2\pi }}{T}, we can calculate time period of particle as T=2πωT = \dfrac{{2\pi }}{\omega }.

Complete step by step answer:
In simple harmonic motion, the velocity of moving particle is given byv=ωA2y2v = \omega \sqrt {{A^2} - {y^2}}
Using above formula, Velocity of particle with displacement is given as v1=ωA2y12{v_1} = \omega \sqrt {{A^2} - y_1^2} ….(i)
And Velocityv2{v_2} of particle with displacement y2{y_2}is given as v2=ωA2y22{v_2} = \omega \sqrt {{A^2} - y_2^2} ….(ii)
On squaring equations (i) and (ii), we get
v12=ω2(A2y12)v_1^2 = {\omega ^2}\left( {{A^2} - y_1^2} \right) ….(iii)
v22=ω2(A2y22)v_2^2 = {\omega ^2}\left( {{A^2} - y_2^2} \right) ….(iv)
Subtracting (iii) from (iv), we get
v22v12=ω2(A2y22)ω2(A2y12)v_2^2 - v_1^2 = {\omega ^2}\left( {{A^2} - y_2^2} \right) - {\omega ^2}\left( {{A^2} - y_1^2} \right)
v22v12=ω2A2ω2y22ω2A2+ω2y12\Rightarrow v_2^2 - v_1^2 = {\omega ^2}{A^2} - {\omega ^2}y_2^2 - {\omega ^2}{A^2} + {\omega ^2}y_1^2
v22v12=ω2[y12y22]\Rightarrow v_2^2 - v_1^2 = {\omega ^2}\left[ {y_1^2 - y_2^2} \right]
ω2=v22v12y12y22\Rightarrow {\omega ^2} = \dfrac{{v_2^2 - v_1^2}}{{y_1^2 - y_2^2}}
ω=v22v12y12y22\therefore \omega = \sqrt {\dfrac{{v_2^2 - v_1^2}}{{y_1^2 - y_2^2}}}
Here is the angular frequency of particles in Simple Harmonic Motion. It is given by ω=2πT\omega = \dfrac{{2\pi }}{T}
Hence, time period is given by, T=2πωT = \dfrac{{2\pi }}{\omega }
T=2πv22v12y12y22T = \dfrac{{2\pi }}{{\sqrt {\dfrac{{v_2^2 - v_1^2}}{{y_1^2 - y_2^2}}} }}
T=2πy12y22v22v12\Rightarrow T = 2\pi \sqrt {\dfrac{{y_1^2 - y_2^2}}{{v_2^2 - v_1^2}}}
\therefore, Time period is T=2πy12y22v22v12T = 2\pi \sqrt {\dfrac{{y_1^2 - y_2^2}}{{v_2^2 - v_1^2}}}

Hence, the correct answer is option (D).

Additional information:
In SHM, on the moving object, the restoring force occurs. This force is directly proportional to the displacement. The restoring force always acts towards the object's equilibrium position. It results in an oscillation. Simple harmonic motion is used to define a mathematical model for different types of motion. Most terminologies used for SHM are time period (or simply we write period), angular frequency, amplitude, displacement.

Note: A particle is moving in simple harmonic motion with 2 different velocities, So students should be clear that the angular frequency and amplitude will be the same. Students can see all the options. We can see that amplitude A is not included. So when they solve equations of velocities, they should remove amplitude.