The bob of a stationary pendulum is given a sharp hit to impart it a horizontal speed of √(3gl) . Find the angle rotated by the string before it comes slack.
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Let, length of the string = l
bob speed = u =√mgl
{Refer to the attachment}
Now Total mechanical energy
(l+ lcosθ)
(1+cosθ) ---→ eq.(a)
Now consider the force here at the final position.
mv² l = mg.cosθ
v² = lg.cosθ ---→ eq. (b)
Equating eq. (a) & (b) we get.
2gl cosθ =gl.cosθ .
By this we get,
3cos = 1
cosθ =1/3
___________
θ = cos⁻(1/3)
___________
At the time string become slack .
cos(180°-θ) = 1/3
___________
θ= cos⁻(-1/3)
___________
Hope it Helps :-)
bob speed = u =√mgl
{Refer to the attachment}
Now Total mechanical energy
(l+ lcosθ)
(1+cosθ) ---→ eq.(a)
Now consider the force here at the final position.
mv² l = mg.cosθ
v² = lg.cosθ ---→ eq. (b)
Equating eq. (a) & (b) we get.
2gl cosθ =gl.cosθ .
By this we get,
3cos = 1
cosθ =1/3
___________
θ = cos⁻(1/3)
___________
At the time string become slack .
cos(180°-θ) = 1/3
___________
θ= cos⁻(-1/3)
___________
Hope it Helps :-)
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