Time derivatives of polar motion

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SUMMARY

The discussion focuses on deriving the acceleration vector, \(\mathbf{a}\), for a particle moving along the curve defined by \(r = k(1+\cos \theta)\) with constant velocity. The equations of motion are established using polar coordinates, leading to the expression for acceleration: \(\mathbf{a} = (\ddot r - r\dot \theta^2)\mathbf{e_r} + (2\dot r\dot \theta + r\ddot \theta)\mathbf{e_\theta}\). The challenge lies in expressing \(r\) and \(\theta\) in terms of time \(t\) while maintaining constant speed. The participant is advised to utilize the velocity equation to derive a formula for speed and equate it to a constant for further simplification.

PREREQUISITES
  • Understanding of polar coordinates and their derivatives
  • Familiarity with vector calculus and acceleration in polar motion
  • Knowledge of constant speed motion and its implications on kinematic equations
  • Proficiency in differentiating parametric equations with respect to time
NEXT STEPS
  • Develop a formula for speed in polar coordinates using the derived velocity equation
  • Explore the relationship between \(r\) and \(\theta\) under constant speed conditions
  • Investigate the implications of constant velocity on the derivatives of polar coordinates
  • Practice solving similar problems involving acceleration in polar motion
USEFUL FOR

Students and educators in physics, particularly those studying mechanics and polar motion, as well as anyone seeking to deepen their understanding of kinematics in non-linear paths.

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Homework Statement


A particle moves with v=constant along the curve
$$r = k(1+\cos \theta)$$Find ##\mathbf{a}##

Homework Equations


$$ \mathbf{r} = r\mathbf{e_r}$$ $$ \mathbf{v} = \frac{\partial}{\partial t}(r\mathbf{e_r}) $$ $$ \mathbf{a} = \frac{\partial \mathbf{v}}{\partial t} $$ $$\mathbf{\dot e_r}=\dot \theta\mathbf{e_\theta} $$ $$\mathbf{\dot e_\theta}= -\dot \theta\mathbf{e_r} $$

The Attempt at a Solution


$$\mathbf{v} = \dot r\mathbf{e_r}+r\mathbf{\dot e_r} = \dot r\mathbf{e_r} + r\dot \theta\mathbf{e_\theta}$$ $$\mathbf{a} = \ddot r\mathbf{e_r}+\dot r\mathbf{\dot e_r}+\dot r\dot \theta\mathbf{e_\theta}+r\ddot \theta\mathbf{e_\theta}+r\dot \theta\mathbf{\dot e_\theta} $$ $$\mathbf{a} = \ddot r\mathbf{e_r}+\dot r\dot \theta\mathbf{e_\theta}+\dot r \dot \theta\mathbf{e_\theta}+r\ddot \theta\mathbf{e_\theta}-r\dot \theta ^2\mathbf{e_r}$$ $$\mathbf{a} = (\ddot r - r\dot \theta ^2)\mathbf{e_r} + (2\dot r\dot \theta + r\ddot \theta)\mathbf{e_\theta}$$
From here I am having some trouble. I cannot figure out how to get equations for ##r## and ##\theta## in terms of ##t##. I would guess that it has something to do with v being constant. Because r is a cardioid I don't think I can just use ##\theta=t##.
 
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You have not yet used the fact that speed is constant. The first equation in your attempted solution gives the velocity. Use that to develop a formula for the speed and then set that equal to a constant. That should give you something to substitute into your last equation to get rid of some stuff.
 

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