Sotiris Michos
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Homework Statement
I would like to ask a question I was discussing the other day with a friend of mine. Suppose you have a point mass m, sliding on the friction-free curve y = e^{-x} starting from position x(0) = 0 and y(0) = 1 with zero initial velocity. Can we find in closed-form the exact position (x,y) with respect to time?
2. The attempt at a solution
Going down the usual path, from conservation of energy I found that v = \sqrt{2g(1-y)}. Assuming φ is the angle between \vec{v} and the downward vertical direction (the direction of negative ordinates), and using that \dot{x} = v \sin(φ), \dot{y} = v \cos(φ), φ = \tan^{-1}(e^{x}), I reached
\dot{x} = \sqrt{2g}\sqrt{\frac{e^{2x}-e^{x}}{e^{2x}+1}}
\dot{y} = -y\sqrt{2g}\sqrt{\frac{1-y}{1+y^2}}
From these two, I need to solve only one. Choosing the first, separating dx and dy and integrating, yields
\int_0^{x(t)}\sqrt{\frac{e^{2x} + 1}{e^{2x} - e^{x} }}dx = \sqrt{2g}t
However, plugging the integral in the LHS in Mathematica doesn't compute anything, most likely meaning that this integral is not solvable in closed form, let alone invertible in closed-form.
Choosing now the second equation and doing the same yields:
\int_1^{y(t)}\sqrt{\frac{1+y^2}{1 - y}}\frac{dy}{y} = - \sqrt{2g}t
Again, trying to compute the integral in the LHS, gives an assortment of complex elliptic integrals that are gain not invertible in some closed-form. Any thoughts about what can be done?
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