Particle experiencing only an angular force, determine the r dot

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The discussion focuses on determining the relationship between the radial velocity (r') and the radial position (r) of a particle experiencing only an angular force, defined as Fθ = m r' θ'. The participants derive equations from polar coordinates, concluding that the radial acceleration is zero and that the relationship can be expressed as r'' = rθ'^2. The key insight is that the dependence of r' on r can be established through a differential equation, specifically relating r' to r and its derivatives.

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Homework Statement
Consider a particle that feels an angular force only, of the form Fθ = m r' θ'.
Determine the dependence of r' on r.
Relevant Equations
Relevant equations are:
particle acceleration in polar coordinates
Fr = 0
F(theta) = mr'θ'.
Hey, I've been working on this for a couple hours, and still no luck.

Since the force in the radial direction is zero, I set
r'' = rθ'^2.
Then since Fθ = m r' θ' and, since it's in polar coordinates, Fθ = m(2r'θ' + rθ'').
Setting these two equal, I get: -r'θ' = rθ''

At this point, I'm stumped. I try to substitute the angular velocity/ acceleration for something in terms of r, try to integrate, but inevitably I reach a point where I can't integrate anymore.
 
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flinnbella said:
Homework Statement: Consider a particle that feels an angular force only, of the form Fθ = m r' θ'.
Determine the dependence of r' on r.
Relevant Equations: Relevant equations are:
particle acceleration in polar coordinates
Fr = 0
F(theta) = mr'θ'.

Hey, I've been working on this for a couple hours, and still no luck.

Since the force in the radial direction is zero, I set
r'' = rθ'^2.
Then since Fθ = m r' θ' and, since it's in polar coordinates, Fθ = m(2r'θ' + rθ'').
Setting these two equal, I get: -r'θ' = rθ''
You can rewrite that as$$r\ddot \theta + \dot r \dot \theta = 0$$Do you recognise an exact time derivative there?
 
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PS you also have another equation of motion from the ##\hat r## component.
 
PPS is the question to get the dependence of ##\ddot r## on ##r##? I.e. a differential equation for ##r##.
 
PeroK said:
PPS is the question to get the dependence of ##\ddot r## on ##r##? I.e. a differential equation for ##r##.
As far as I can tell it's either what you suggest ( which is very clean ), or you get ##\dot r ## as a function of ##r, \ddot r , \dddot r##.
 
What can be considered "an angular force" in this type of problems?
 
A force that has an angular but no radial component?
 
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kuruman said:
A force that has an angular but no radial component?
So ##\vec F=m\dot r\dot\theta\hat\theta##, right @flinnbella ?
 
haruspex said:
So ##\vec F=m\dot r\dot\theta\hat\theta##, right @flinnbella ?
Yes exactly. There is no radial force and the radial acceleration is zero
 
  • #10
PeroK said:
PPS is the question to get the dependence of ##\ddot r## on ##r##? I.e. a differential equation for ##r##.
No its on the dependence of the radial velocity on the radial position.
 
  • #11
PeroK said:
PPS is the question to get the dependence of ##\ddot r## on ##r##? I.e. a differential equation for ##r##.
It's on r dot dependence on r, not r double dot
 
  • #12
flinnbella said:
It's on r dot dependence on r, not r double dot
It's difficult to know what is required, but if we take ##\frac d {dt} \dot r = \ddot r##, then that gives us a relationship between ##\dot r## and ##r##.

You should be able to make progress in any case, following the conventional approach in these problems (as I hinted at in the posts above).
 
  • #13
flinnbella said:
No its on the dependence of the radial velocity on the radial position.
You may recall ##\ddot x=\dot x\frac{d\dot x}{dx}##.
 
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  • #14
haruspex said:
You may recall ##\ddot x=\dot x\frac{d\dot x}{dx}##.
Behold the power of the Chain Rule!
 
  • #15
erobz said:
Behold the power of the Chain Rule!
Wow, I figured it out, thank you
 
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  • #16
flinnbella said:
Wow, I figured it out, thank you
Thanks! but I’ll forward that to the providers of the key insights @PeroK , @haruspex
 
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