Time derivatives of polar motion

In summary, the problem is to find the acceleration of a particle moving with constant speed along the curve r = k(1+cos θ). Using the equations for position, velocity, and acceleration, the acceleration is found to be (ddot r - rdot θ^2)e_r + (2rdot θ + rddot θ)e_θ. To solve for r and θ in terms of t, we need to use the fact that speed is constant. This can be done by setting the formula for speed equal to a constant, which can then be substituted into the acceleration equation to simplify it.
  • #1
stumpoman
10
1

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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  • #2
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.
 

Related to Time derivatives of polar motion

1. What are time derivatives of polar motion?

Time derivatives of polar motion refer to the rate of change of the Earth's rotation axis and the motion of the Earth's crust. This includes the Chandler wobble, the annual wobble, and the long-term trends of polar motion.

2. How are time derivatives of polar motion measured?

Time derivatives of polar motion are measured using various techniques such as satellite laser ranging, very long baseline interferometry, and global positioning system (GPS) measurements. These techniques allow for precise measurements of the Earth's rotation and polar motion.

3. What causes time derivatives of polar motion?

There are several factors that contribute to time derivatives of polar motion. These include mass redistribution within the Earth, atmospheric and oceanic processes, and changes in the Earth's climate. These factors all affect the distribution of mass within the Earth, which in turn affects the Earth's rotation and polar motion.

4. How do time derivatives of polar motion impact the Earth's climate?

Time derivatives of polar motion can affect the Earth's climate in various ways. Changes in polar motion can alter the distribution of solar energy on the Earth's surface, which can lead to changes in global climate patterns. Additionally, changes in polar motion can also affect sea level and ocean currents, which can impact weather patterns and climate across the globe.

5. Can time derivatives of polar motion be predicted?

While there are models that can predict short-term variations in polar motion, long-term predictions are more challenging due to the complexity of the Earth's systems. However, ongoing research and advancements in technology are helping scientists improve their understanding and prediction of time derivatives of polar motion.

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