How Do You Calculate Time Along a Path in Polar Coordinates?

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Homework Help Overview

The problem involves calculating the time taken to move along a path defined in polar coordinates, specifically given by the equation r=a*cos²(θ). The original poster seeks to understand the integration method required to find this time between two angles, given a velocity function along the path.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the need for integration to solve the problem and explore the relationship between velocity and time along the path. There are attempts to express time in terms of the integral of velocity and differential length, with questions about the assumptions made regarding the path's curvature.

Discussion Status

Participants are actively engaging with the problem, providing insights into the equations for differential length and tangential velocity. Some guidance has been offered regarding the correct formulation of the differential distance along the trajectory, indicating a productive direction in the discussion.

Contextual Notes

There are constraints regarding the need to show attempts before receiving help, and participants are questioning the validity of their assumptions about the path's geometry and the application of certain formulas.

vmedica
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Homework Statement



I have a path defined in polar coordiantes defined as r=a*cos2(θ). I also have the velocity along this path as a function of θ. I want to find the time take to move between two given angles on the path.2. The attempt at a solution

I know that this problem will involve some kind of integration but what is the general method behind solving this kind of problem.
 
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$$ \vec{v} = \frac {d\vec{R}} {dt} = \frac {d\vec{R}} {d\theta} \frac {d\theta} {dt } $$
 
The rules are that you need to show some attempt to solve the problem before anyone can help you. So show us what you have tried so far.
 
Well my idea is that since I have the velocity of the particle in the direction of the path, then would the time just be ∫(a*cos2(θ)/v(θ))dθ integrated between the two angles I want ( f(v) is the velocity along the path as a function of theta). The main problem is see with this is that r dθ is for a circular loop but can I assume this because dθ is very small.
 
vmedica said:
Well my idea is that since I have the velocity of the particle in the direction of the path, then would the time just be ∫(a*cos2(θ)/v(θ))dθ integrated between the two angles I want ( f(v) is the velocity along the path as a function of theta). The main problem is see with this is that r dθ is for a circular loop but can I assume this because dθ is very small.

This isn't quite right, but you are on the right track. Let me help you. If the particle trajectory is arbitrary, what is the equation for a differential length ds along the trajectory in terms of r, dr, and dθ? What is the equation for the tangential velocity v in terms of ds and dt?
 
Differential length is √(r2+(dr/dθ)2).

Do you mean the tangential component of the velocity? For that, I get √(ds2-dr2). (Using v=r dθ and ds2=(r dθ)2+dr2).

Or do you mean the tangent to the curve at that point, if ds is a straight line at that point, then v=ds/dt. This looks better, so would time just be ∫ds/v= ∫√(r2+(dr/dθ)2)/v dθ , where v is the velocity along the curve?
 
vmedica said:
Differential length is √(r2+(dr/dθ)2).

Do you mean the tangential component of the velocity? For that, I get √(ds2-dr2). (Using v=r dθ and ds2=(r dθ)2+dr2).

Or do you mean the tangent to the curve at that point, if ds is a straight line at that point, then v=ds/dt. This looks better, so would time just be ∫ds/v= ∫√(r2+(dr/dθ)2)/v dθ , where v is the velocity along the curve?

√(r2+(dr/dθ)2) isn't quite right. The differential distance ds along the trajectory is this multiplied by dθ. [tex]ds=\sqrt{(dr)^2+(rd\theta)^2}[/tex]

So, [tex]dt=\frac{\sqrt{(\frac{dr}{d\theta})^2+r^2}}{v(\theta)}d\theta[/tex]
 
That makes sense now. Thank you for your help.
 

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