Question #73380

two particle A and B executing SHM along same straight line with same amplitude and same mean position A start its motion from mean position and move toward positive extreme while B starts from negative extreme position Angular frequency of A is Wa and that of B is Wb choose the incorrect statment
A)if Wa =2Wb then when they meet first their velocity will be zero
B)ifWa>2Wb then when they meet first time their velocity are in same direction
C)ifWa<2Wb then when they meet their velocity will be in same direction
D)their velocity when they meet does not depend on W
1

Expert's answer

2018-02-12T07:34:08-0500

Answer on Question #73380, Physics / Mechanics | Relativity

Question. Two particle AA and BB executing SHMSHM along same straight line with same amplitude and same mean position. AA starts its motion from mean position and moves toward positive extreme while BB starts from negative extreme position. Angular frequency of AA is ωA\omega_A and that of BB is ωB\omega_B choose the incorrect statement

A) if ωA=2ωB\omega_A = 2\omega_B then when they meet first their velocity will be zero.

B) if ωA>2ωB\omega_A > 2\omega_B then when they meet first time their velocity are in same direction.

C) if ωA<2ωB\omega_A < 2\omega_B then when they meet their velocity will be in same direction.

D) their velocity when they meet does not depend on ω\omega.

Solution.

A) if ωA=2ωB\omega_A = 2\omega_B then when they meet first their velocity will be zero.

Assume that


xA(t)=sin(ωAt),x_A(t) = \sin(\omega_A t),xB(t)=sin(ωBtπ2)x_B(t) = \sin\left(\omega_B t - \frac{\pi}{2}\right)


So


vA(t)=dxA(t)dt=ωAcos(ωAt),v_A(t) = \frac{dx_A(t)}{dt} = \omega_A \cos(\omega_A t),vB(t)=dxB(t)dt=ωBcos(ωBtπ2),v_B(t) = \frac{dx_B(t)}{dt} = \omega_B \cos\left(\omega_B t - \frac{\pi}{2}\right),


If xA(t)=xB(t)x_A(t) = x_B(t) and ωA=2ωB\omega_A = 2\omega_B then


sin(ωAt)=sin(ωBtπ2)sin(2ωBt)=sin(ωBtπ2)\sin(\omega_A t) = \sin\left(\omega_B t - \frac{\pi}{2}\right) \rightarrow \sin(2\omega_B t) = \sin\left(\omega_B t - \frac{\pi}{2}\right) \rightarrowsin(2ωBt)sin(ωBtπ2)=0\sin(2\omega_B t) - \sin\left(\omega_B t - \frac{\pi}{2}\right) = 0


The solution of this equation is ωBt=2πn3+π2\omega_B t = \frac{2\pi n}{3} + \frac{\pi}{2}, nZn \in \mathbb{Z}. Hence


vA(t)=ωAcos(ωAt)=2ωBcos(2ωBt)=2ωB.v_A(t) = \omega_A \cos(\omega_A t) = 2\omega_B \cos(2\omega_B t) = -2\omega_B.vB(t)=ωBcos(π2π2)=ωB.v_B(t) = \omega_B \cos\left(\frac{\pi}{2} - \frac{\pi}{2}\right) = \omega_B.


In fig. ωB=3\omega_{B} = 3 rad/s² and ωA=6\omega_{A} = 6 rad/s².



Answer. The statement is incorrect.

B) If ωA>2ωB\omega_{A} > 2\omega_{B} then when they meet first time their velocity are in same direction.



Answer. The statement is incorrect.

C) if ωA<2ωB\omega_{A} < 2\omega_{B} then when they meet their velocity will be in same direction.



Answer. The statement is correct.

D) Their velocity when they meet does not depend on ω\omega .

The velocity when they meet depend on ω\omega (see A)).

Answer. The statement is incorrect.

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