ApeXaviour
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I'm doing these examinations but the lecturer has changed one or two of the questions since I originally sat the course so they are not in my notes how to approach. This is an example of one he changed from a tutorial sheet he gave out a few months back"A particle acted upon by a central attractive force u^{3}\mu is projected with a velocity \frac{\sqrt{\mu}}{a} at an angle of \frac{\pi}{4} with its initial distance a from the centre of the force; show that its orbit is givin by r=ae^{-\theta} "
I'd have already derived the formula \frac{d^{2}u}{d\theta^{2}}+u=\frac{F(\frac{1}{u})}{h^{2}u^{2}} where r^{2}\dot{\theta}=h and u=\frac{1}{r}
But I'm used to doing these types of problems where the particle is projected from an apse. Where I get stuck is when I've gotten it down to the differential equation solution I have:
u=Ae^{\theta}+Be^{-\theta}. When \theta=\frac{\pi}{4}; u=\frac{1}{a}. So I've got Ae^{\frac{\pi}{4}}+Be^{-\frac{\pi}{4}}=\frac{1}{a} But now what? How do I solve for A and B? Usually I'd be able to say that \frac{du}{d\theta}=0 but since this isn't at an apse I can't do that (at least I don't think I can). So how can I get my second simultaneous equation to solve the arbitrary constants A and B?
Thanks
-Declan
I'd have already derived the formula \frac{d^{2}u}{d\theta^{2}}+u=\frac{F(\frac{1}{u})}{h^{2}u^{2}} where r^{2}\dot{\theta}=h and u=\frac{1}{r}
But I'm used to doing these types of problems where the particle is projected from an apse. Where I get stuck is when I've gotten it down to the differential equation solution I have:
u=Ae^{\theta}+Be^{-\theta}. When \theta=\frac{\pi}{4}; u=\frac{1}{a}. So I've got Ae^{\frac{\pi}{4}}+Be^{-\frac{\pi}{4}}=\frac{1}{a} But now what? How do I solve for A and B? Usually I'd be able to say that \frac{du}{d\theta}=0 but since this isn't at an apse I can't do that (at least I don't think I can). So how can I get my second simultaneous equation to solve the arbitrary constants A and B?
Thanks
-Declan
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