How to find the acceleration with polar coordinates?

AI Thread Summary
To find the acceleration of the carriage P in polar coordinates, the velocity is expressed as v = bω/sin(θ). The acceleration requires differentiating this velocity with respect to time, considering both r and θ as functions of time. The correct expression for acceleration can be derived by applying the chain rule and recognizing that as r changes, θ also varies with time. A relationship involving r and θ, specifically r*cos(θ) = h, can be differentiated to find dθ/dt, which can then be substituted into the acceleration formula. This approach leads to the correct answer, confirming the importance of considering both variables in motion.
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Homework Statement



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The quality of the image is bad so here's the statement:

For an interval of motion the drum of radius b turns clockwise at a constant rate ω in radians per second and causes the carriage P to move to the right as the unwound length of the connecting cable is shortened. Use polar coordinates r and θ and serive expressions for the velocity v and acceleration a of P in the horizontal guide in terms of the angle θ. Check your solution with time of the relation x2+h2=r2

Homework Equations



I first found that the velocity of the carriage is v=bω/sin(θ)

The Attempt at a Solution



I attempted to directly derivate the equation which give me -bωcos(θ)/sin2(θ)

However, in the book answers, the answer is supposer to be b2ω2/h *cot3(θ).

I think I have to do something with the vectors, like derivate v=vrer + vθeθ but I don't understand much.
 
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It seems to me that you just forgot a term in the chain rule to differentiate your expressior for the speed. Realize that as r is changing, so is \theta, so \theta is also a function of time.

You have v = -\dfrac{b\omega}{\sin{\theta}}

a=\dfrac{dv}{dt} = \dfrac{b\omega\cos{\theta}}{\sin{\theta}^2}\dfrac{d\theta}{dt}

There is probably a simpler way to do this, but to obtain \frac{d\theta}{dt} you can realize that r*\cos{\theta} = h, where h is a constant. If you differentiate both sides, you get

\dfrac{dr}{dt}*cos{\theta} + r(-\sin{\theta})\dfrac{d\theta}{dt} = 0

You can solve for \dfrac{d\theta}{dt} and plug it into the expression for a, it gives you the right answer :) Realize that \frac{dr}{dt} = -b\omega, since it is simply the rate at which the rope is being pulled.

Did I make any sense? :P
 
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