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Hi Ignoblius- I'd be interested to know what the course is that you are studying (Physics degree?).
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Hi Ignoblius
Yes but that's no mean task, because the only way you can solve for r is by using setting a value for t and then using the Newton-Raphson numerical method to iterate to the corresponding value of r. By the way just one small correction to your last post: theta=pi/2 at r=0 theta=0 at r=R You could use a spreadsheet to do the Newton-Raphson or just produce a spreadsheet and do the calculation as I mentioned in my pdf. Here's a link to a spreadsheet which does it: https:/ Vasco |
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Also should be r=Rcos^2(theta) in you last post.
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Question Author
I graphed out
t= √(R³/2K) * [acos (√r / √R) + √(r(R-r)) / R] then flipped it about to get an image of the inverse function. I can't put a graphic into this post but what I get looks like a half-cycle of a periodic function. It is what you would get if particle B passed through center point A without collision, reaching apogee at -R and falling back to A again. By linking the curve with its mirror image to get the complete cycle, the result looks like a rectangular waveform with the flats & corners rounded. The movement of particle B seems like an elliptical orbit with a minor axis of zero. If it's a periodic waveform a Fourier transform is possible. The result can be differentiated to get v(t) and a(t). |
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Its a cardioid if you adjust the scales of r and t as follows:
x can be written as: x=R/2*(1+cos2 theta) and t=sqrt(R^3/(2K))/2*(2 theta+sin2 theta) =R/2*sqrt(R/(2K))*(2 theta+sin2 theta) So if we define T as t/sqrt(R/(2K)) which is just a scaling factor then if we let a=R/2 then X=a(1+cos2 theta) and T=a(2 theta+sin2 theta) and this is the equation of a cardioid. |
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