A particle follows a spiral orbit given by r = c (theta)2 under an unknown force law. Prove that such an orbit is possible in a central field. Also find the force law?
Answer
u="\\frac{1}{r}=\\frac{1}{c\\theta^2}"
For finding force law
"\\frac{d^2u}{d\\theta^2}+u=-\\frac{Fm}{l^2u^2}"
Putting value of
"\\frac{d^2u}{d\\theta^2}=\\frac{6}{c\\theta^4}"
And u in above equation
"\\frac{6}{c\\theta^4}+\\frac{1}{c\\theta^2}=-\\frac{Fm}{l^2u^2}"
Changing in r form
Then force law become
"F=-\\frac{m}{l^2}(6c+r)"
Comments
Leave a comment