Particle under central force with u(θ) = 1/r substitution

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Since r is periodic w.r.t. the angle, the orbit has to be closed. But it is not repeated every 120 degrees. It is repeated every 360 degrees.
 
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voko said:
Since r is periodic w.r.t. the angle, the orbit has to be closed. But it is not repeated every 120 degrees. It is repeated every 360 degrees.

Maybe I misused the word 'repeated' and I see what you mean. This is the last part of this question:

The angle between successive maxima and minima is called the apsidal angle. Derive an expression for ##dr/d\theta = \dot{r}/\dot{\theta}## by extracting ##\dot{r}## from the expression for the energy and using ##\dot{\theta} = h/r^2##. Use this expression to determine the apsidal angle and compare with your result previously.

The energy is conserved so I was given that ##E = T + U,\,U = mk[\frac{9}{8} a/r^2 - 3/r]##. T = 0 initially (since ##\dot{r} ##= 0) and so E = U = -15mk/8a, with the condition r(0) = a.

My problem is that when I rearrange for ##\dot{r}##, it appears I will have a negative under the square root. I believe what I am rearranging is the following: $$-\frac{15}{8} mk/a = \frac{m}{2}\dot{r}^2 + mk[\frac{9}{8}\frac{a}{r^2} - \frac{3}{r}]$$ Rearranging gives $$\dot{r} = \sqrt{-\frac{15}{8} mk/a - 3mk/r - 9mka/8r^2}$$ which is a negative under the square root.

EDIT: The potential U was given to us in the question as ##mk [\frac{9}{8} a/r^2 - 3/r]##
 
Without analyzing it further, there is clearly a sign error in the 1/r term after rearranging.
 
voko said:
Without analyzing it further, there is clearly a sign error in the 1/r term after rearranging.

I get the apsidal angle to be ##\theta = \frac{2 \pi}{3}##. This agrees with the difference between the maxima and minima earlier. Just one more question: what exactly does the question mean by the geometrical significance of the max and min r? I would say that the particle can never go below 3a/5 and never beyond a, but this seems to be more of a physical significance rather than the geometry.
 
The only geometrical statement that I could make would involve the other two trajectories, but I am not sure if this is what is needed (since they don't mention the other two orbits in the question)
 
Perhaps you could compare that to an elliptical orbit.
 
voko said:
Perhaps you could compare that to an elliptical orbit.

So maybe that the particle on the elliptical orbit has the same r(min) and r(max)
 
The apsidal angle is defined as the angle between successive minima and maxima so the answer was pi/3. We just defined the apsidal angle properly today in lectures and the method used to obtain the apsidal angle was an integral. I understand this method. The way I found the angle (which I did before seeing the integral method) was as follows:

Since we have a functional form for r, I just subbed it into the resulting energy equation. I then solved for r'(θ) =0. This gave me the n2π/3. Since we know this corresponds to maxima as shown earlier, and since we know there is a change in concavity between two maxima, then this must correspond to a minima (as my sketch of the orbit showed). Hence to get the apsidal angle I would then divide by 2 to get nπ/3. Want the difference between successive max/min so I take the angle to be π/3.

Is this okay? (Very recently, I have become aware that some of the TAs at my university mark like computers and I think the method they will mark against will be via the integral). So if you think it is okay, I will argue will them. Obviously, I am aware that my method is not the most general, but I did what I did before going over the integral method.

Many thanks.
 
There is nothing wrong with your method. You found an explicit expression for minima and maxima, and that is enough to find the apsidal angle. If there was not a specific requirement to use a particular method to solve the problem, you should be fine. After all, this is physics, and there is usually more than one way to solve a problem.
 
Thanks voko.