I am investigating the theory of a radial (not a polar) planimeter - when tracing a closed contour with the "pole" of the device outside of the contour (normally, the "pole" would be inside the contour).
This has led me to this horrible expression below, whilst trying to evaluate a line integral - and I have been unable to progress beyond it...
$$ \int_0^{2\pi } \frac{r\ldotp \mathrm{cos}\left(t\right)\ldotp \left(a+r\ldotp \mathrm{cos}\left(t\right)\right)}{\sqrt{{\left(a+r\ldotp \mathrm{cos}\left(t\right)\right)}^2 +{\left(b+r\ldotp \mathrm{sin}\left(t\right)\right)}^2 }}+\frac{r\ldotp \mathrm{sin}\left(t\right)\ldotp \left(b+r\ldotp \mathrm{sin}\left(t\right)\right)}{\sqrt{{\left(a+r\ldotp \mathrm{cos}\left(t\right)\right)}^2 +{\left(b+r\ldotp \mathrm{sin}\left(t\right)\right)}^2 }}\mathrm{dt} $$ Does anyone have any suggestions about how I might proceed with the solution to this? (Wolfram times out and so does the rudimentary symbolic processor which I have access to).
I therefore reverted to a numerical approach and found that the results appear to be physically plausible (also nicely confirmed by measurements using an actual instrument), but I want to find the analytical solution as this will obviously provide much more insight into the underlying process. Of course, I realise that there may not be an analytical solution...
Thanks for looking.