A child pulls a loaded sledge across level snow by means of a rope. The rope is inclined at \(\theta\) radians to the horizontal (see the diagram).
The smallest tension, \(F\) newtons, in the rope that keeps the sledge moving is modelled by
\(F(\theta)=\dfrac{k}{\cos\theta+\mu\sin\theta},\quad 0\leq\theta\leq\dfrac{\pi}{2},\)
where \(k\) and \(\mu\) are positive constants. When the rope is horizontal, \(F=240\).
The tension is also \(240\) newtons when \(\theta=\dfrac{\pi}{3}\).
The tension takes its least value when the rope is inclined at \(\beta\) radians to the horizontal, for some angle \(\beta\) with \(0<\beta<\dfrac{\pi}{2}\).
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