M3 June 2013 (R) Q5
5.

Part of a hollow spherical shell, centre \(O\) and radius \(r\), forms a bowl with a plane circular rim. The bowl is fixed to a horizontal surface at \(A\) with the rim uppermost and horizontal.
The point \(A\) is the lowest point of the bowl. The point \(B\), where \(\angle AOB = \alpha\) and \(\tan\alpha = \dfrac{3}{4}\), is on the rim of the bowl, as shown in Figure 2. A small smooth marble \(M\) is placed inside the bowl at \(A\), and given an initial horizontal speed \(\sqrt{(gr)}\). The motion of \(M\) takes place in the vertical plane \(OAB\).
After leaving the surface of the bowl at \(B\), \(M\) moves freely under gravity and first strikes the horizontal surface at the point \(C\). Given that \(r = 0.4\) m,
| Scheme | Marks |
|---|---|
| Use of Energy at A = energy at B | |
| \(\dfrac{1}{2}mu^2 = \dfrac{1}{2}mv^2 + mgh,\ \ \dfrac{1}{2}mgr = \dfrac{1}{2}mv^2 + mg \times r(1 - \cos\alpha)\) | M1 A1A1 |
| \(= \dfrac{1}{2}mv^2 + mg \times r \times \dfrac{1}{5}\) | |
| \(v^2 = gr - \dfrac{2gr}{5} = \dfrac{3gr}{5}\) | |
| \(v = \sqrt{\dfrac{3gr}{5}}\) *AG* | A1 |
| (4) |
| Scheme | Marks |
|---|---|
| v1 Horizontal component of speed at \(B\) and at \(C\) = their \(v\cos\theta\) | M1 |
| Vertical component of speed at B = their \(v\sin\theta\) | M1 |
| Conservation of energy gives speed at C \(= \sqrt{\dfrac{2g}{5}}\) | |
| Vertical component of speed at C \(= \sqrt{\dfrac{2g}{5} - \dfrac{16 \times 6g}{25^2}} \approx 1.5539..\) | M1A1 |
| \(v = u + at \Rightarrow\) \(t = \dfrac{1.5539\ldots + 0.92017\ldots}{g} \approx 0.252..\) seconds | M1A1 |
| Horizontal distance \(= \dfrac{3}{5} \times 0.4 + 1.22689.. \times 0.252\ldots = 0.55\) (m) | M1A1 |
| (8) | |
| (12 marks) |
(b) v2
| Horizontal component of speed at \(B\) and at \(C\) = their \(v\cos\theta\) | M1 |
| Vertical component of speed at B = their \(v\sin\theta\) | M1 |
| \(s = ut + \dfrac{1}{2}at^2:\ -\dfrac{1}{5} \times 0.4 = -\dfrac{2}{25} = \sqrt{\dfrac{6g}{25}} \times \dfrac{3}{5}t - \dfrac{1}{2}gt^2\) | M1A1 |
| \(4.9t^2 - .92017..t - 0.08 = 0\) | |
| \(t = \dfrac{0.920 + \sqrt{0.920^2 + 0.32 \times 4.9}}{9.8} = 0.252\ldots\ldots\) | M1A1 |
| Horizontal distance \(= \dfrac{3}{5} \times 0.4 + 1.22689.. \times 0.252\ldots = 0.55\) (m) | M1A1 |
(b) v3
| Horizontal component of speed at \(B\) and at \(C\) = their \(v\cos\theta\) | M1 |
| Vertical component of speed at B = their \(v\sin\theta\) | M1 |
| \(s = ut + \dfrac{1}{2}at^2:\ -\dfrac{1}{5} \times 0.4 = -\dfrac{2}{25} = \sqrt{\dfrac{6g}{25}} \times \dfrac{3}{5}t - \dfrac{1}{2}gt^2\) | M1A1 |
| \(4.9t^2 - .92017t - 0.08 = 0\) | |
| Horizontal distance from B \(= 1.22689\ldots \times t = x\) | |
| Form quadratic in x by substituting for \(t\) above | M1 |
| \(3.255x^2 - 0.75x - 0.08 = 0\) | |
| \(x = \dfrac{0.75 + \sqrt{0.75^2 + 4 \times 3.255 \times 0.08}}{2 \times 3.255} = 0.3097\ldots\) | M1A1 |
| Horizontal distance \(= \dfrac{3}{5} \times 0.4 + 0.3097\ldots = 0.55\) (m) | A1 |