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A particle initially at rest at point A(0, 0) slides down from a frictionless wire in a vertical plane to another point \(B(y_{0}, z_{0})\) under the influence of gravity. Then according to principle of variation, the minimum time \((\tau)\) taken by particle can be evaluated using the expression :

(where, \(z' = \frac{dz}{dy}\))

  • A.\(\frac{1}{\sqrt{2g}}\int_{z=0}^{z_{0}} \frac{\sqrt{1+z'^{2}}}{\sqrt{z}}\,dy\)
  • B.\(\frac{1}{\sqrt{2g}}\int_{z=0}^{z_{0}} \frac{\sqrt{1-z'^{2}}}{\sqrt{z}}\,dy\)
  • C.\(\frac{1}{\sqrt{2g}}\int_{z=0}^{z_{0}} \frac{\sqrt{1+z'^{2}}}{\sqrt{z'}}\,dy\)
  • D.\(\frac{1}{\sqrt{2g}}\int_{z=0}^{z_{0}} \frac{\sqrt{1-z'^{2}}}{\sqrt{zz'}}\,dy\)

Answer: A

The time is \(\frac{1}{\sqrt{2g}}\int \frac{\sqrt{1+z'^{2}}}{\sqrt{z}}\,dy\).

This is the brachistochrone set-up, with \(z\) measured downward from the starting point. Starting from rest, energy conservation gives the speed after falling a height \(z\), and the arc length element is written in terms of \(z' = dz/dy\):

\[ \begin{aligned} v &= \sqrt{2gz} \\ ds &= \sqrt{1 + z'^{2}}\,dy \\ \tau &= \int\frac{ds}{v} \\ &= \frac{1}{\sqrt{2g}}\int\frac{\sqrt{1+z'^{2}}}{\sqrt{z}}\,dy \end{aligned} \]

The calculus of variations then minimises this functional. The arc length always has \(1 + z'^{2}\) (Pythagoras), so the options with \(1 - z'^{2}\) are wrong, and the speed depends on the height fallen \(z\), not on the slope \(z'\), which rules out \(\sqrt{z'}\) and \(\sqrt{zz'}\) in the denominator.

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