Find the acceleration vector in terms of u subscript r and u subscript

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To find the acceleration vector in terms of u subscript r and u subscript theta, start by correctly differentiating the radial function r = a(4 - cos(θ)). The derivative dr/dθ is a sin(θ), leading to dr/dt = 6a sin(θ) when applying the chain rule with dθ/dt = 6. The acceleration vector is expressed as <d²x/dt², d²y/dt²>, with x and y defined in terms of r and θ. The discussion also seeks clarification on the meanings of u subscript r and u subscript theta, indicating a need for further explanation of these terms in the context of polar coordinates. Understanding these concepts is essential for completing the acceleration vector calculation.
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Find the acceleration vector in terms of u subscript r and u subscript \theta
r = a(4-cos\theta) and d\theta/dt = 6

Im pretty sure to take the derivative:

r' = a(4+sin\theta)
r" = a(4+cos\theta)

what should i do next?
 
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Your derivative is not quite right- dr/d\theta= asin(\theta)- the derivative of "4" is 0 since it is a constant. Then, by the chain rule, dr/dt= asin(\theta) d\theta/dt= 6a sin(\theta).

The acceleration vector is \left&lt;d^2x/dt^2, d^2y/dt^2\right&gt;

Of course, x= r cos(\theta) and y= r sin(\theta) so that dx/dt= (dr/dt)cos(\theta)- rsin(\theta),
dy/dt= (dr/dt)sin(\theta)+ rcos(\theta),
d^2x/dt^2= (d^2r/dt^2)cos(\theta)- 2(dr/dt)sin(\theta)- rcos(\theta),
and
d^2y/dt^2= (d^2r/dt^2)sin(\theta)+ 2(dr/dt)cos(\theta)- rsin(\theta)

You were given d\theta/dt before and I gave you dr/dt above.
 


I appreciate that, but is there more to it.

I don't perfer the answer, but can you guide me through it.

What does it mean u subscript r and u sunbscript theta?
 
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