ehild
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Abdul Quadeer said:Let the length of the plank be 2l (for simplicity) and let it make an angle θ with the horizontal when normal force by the vertical wall is 0.
1. Energy Conservation-
ω2 = 3g/2l (sinΦ - sinθ), where Φ is the initial angle of the base with horizontal.
Correct so far, but I but I can not follow you after. I write the details to get the angular acceleration
The angular acceleration is obtained by derivation of
ω2=3g/(2L) (sinΦ - sinθ). *
2ω dω/dt=-3g/(2L)(cosθ)ω --->dω/dt=-3g/(4L)cosθ. **
N=0 means that the horizontal acceleration of the centre of mass is zero. The x coordinate of the CM is xcm=L(cosθ), vcm=-Lω(sinθ) and
acm=-L*(ω2cosθ +dω/dt sinθ ).***
acm=0 means that dω/dt =-ω2cotθ, the same you got.
Substituting (*) for ω2 and (**) for dω/dt in (***) for the horizontal acceleration, you get the angle when the contact is lost.
I do not understand the signs in your torque method. Show what you consider positive directions. Also, dω/dt is missing from your equation for N2. And you got an expression (*) for ω2 already, what are these different new ones?
ehild
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