OCR M3 2013 June — Question 5 10 marks

Exam BoardOCR
ModuleM3 (Mechanics 3)
Year2013
SessionJune
Marks10
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicCircular Motion 2
TypeParticle on outer surface of sphere
DifficultyStandard +0.3 This is a standard M3 circular motion problem requiring energy conservation and the condition for leaving the surface (N=0). Part (i) is a show-that requiring straightforward application of these principles, parts (ii) and (iii) follow directly from the result. Slightly easier than average due to the guided structure and standard techniques.
Spec6.05d Variable speed circles: energy methods6.05e Radial/tangential acceleration

5 \includegraphics[max width=\textwidth, alt={}, center]{3e8248ca-74f1-443f-a5db-d7da532d2815-3_449_442_1281_794} A fixed smooth sphere of radius 0.6 m has centre \(O\) and highest point \(T\). A particle of mass \(m \mathrm {~kg}\) is released from rest at a point \(A\) on the sphere, such that angle \(T O A\) is \(\frac { \pi } { 6 }\) radians. The particle leaves the surface of the sphere at \(B\) (see diagram).
  1. Show that \(\cos T O B = \frac { \sqrt { 3 } } { 3 }\).
  2. Find the speed of the particle at \(B\).
  3. Find the transverse acceleration of the particle at \(B\).

Question 5(i):
AnswerMarks Guidance
AnswerMarks Guidance
Use of energy equation at \(A\) and \(B\)M1 3 terms needed; allow sign error, missing \(m/g/r\)
\(mg0.6\cos\frac{\pi}{6} = mg0.6\cos\theta + \frac{1}{2}mv^2\)A1 Allow if \(\theta\) replaced by \(\varphi + \pi/6\)
\(F = ma\) radiallyM1 Allow sign error, missing \(m/g\)
\(mg\cos\theta - R = \frac{mv^2}{0.6}\)A1
Use of \(R = 0\)M1 May be incorporated in previous step
\(\cos TOB = \frac{\sqrt{3}}{3}\) AGA1 Completely correct; not given if decimals used for angle
[6]
Question 5(ii):
AnswerMarks Guidance
AnswerMarks Guidance
Use of \(\frac{\sqrt{3}}{3}\) in 'correct' equation in (i)M1 \(mg0.6\cos\frac{\pi}{6} = mg0.6 \times \frac{\sqrt{3}}{3} + \frac{1}{2}mv^2\) or \(mg\frac{\sqrt{3}}{3} = \frac{mv^2}{0.6}\); equation must have gained M1 in (i) but allow restart here
\(1.84\ \text{ms}^{-1}\)A1
[2]
Question 5(iii):
AnswerMarks Guidance
AnswerMarks Guidance
Use of \(F = ma\) tangentiallyM1 \(mg\sin\theta = ma\) seen; allow missing \(m/g\), \(-\) sign; allow M1 if angular accel found
\(8.00\ \text{ms}^{-2}\)A1
[2]
## Question 5(i):

| Answer | Marks | Guidance |
|--------|-------|----------|
| Use of energy equation at $A$ and $B$ | M1 | 3 terms needed; allow sign error, missing $m/g/r$ |
| $mg0.6\cos\frac{\pi}{6} = mg0.6\cos\theta + \frac{1}{2}mv^2$ | A1 | Allow if $\theta$ replaced by $\varphi + \pi/6$ |
| $F = ma$ radially | M1 | Allow sign error, missing $m/g$ |
| $mg\cos\theta - R = \frac{mv^2}{0.6}$ | A1 | |
| Use of $R = 0$ | M1 | May be incorporated in previous step |
| $\cos TOB = \frac{\sqrt{3}}{3}$ AG | A1 | Completely correct; not given if decimals used for angle |
| **[6]** | | |

## Question 5(ii):

| Answer | Marks | Guidance |
|--------|-------|----------|
| Use of $\frac{\sqrt{3}}{3}$ in 'correct' equation in (i) | M1 | $mg0.6\cos\frac{\pi}{6} = mg0.6 \times \frac{\sqrt{3}}{3} + \frac{1}{2}mv^2$ or $mg\frac{\sqrt{3}}{3} = \frac{mv^2}{0.6}$; equation must have gained M1 in (i) but allow restart here |
| $1.84\ \text{ms}^{-1}$ | A1 | |
| **[2]** | | |

## Question 5(iii):

| Answer | Marks | Guidance |
|--------|-------|----------|
| Use of $F = ma$ tangentially | M1 | $mg\sin\theta = ma$ seen; allow missing $m/g$, $-$ sign; allow M1 if angular accel found |
| $8.00\ \text{ms}^{-2}$ | A1 | |
| **[2]** | | |
5\\
\includegraphics[max width=\textwidth, alt={}, center]{3e8248ca-74f1-443f-a5db-d7da532d2815-3_449_442_1281_794}

A fixed smooth sphere of radius 0.6 m has centre $O$ and highest point $T$. A particle of mass $m \mathrm {~kg}$ is released from rest at a point $A$ on the sphere, such that angle $T O A$ is $\frac { \pi } { 6 }$ radians. The particle leaves the surface of the sphere at $B$ (see diagram).\\
(i) Show that $\cos T O B = \frac { \sqrt { 3 } } { 3 }$.\\
(ii) Find the speed of the particle at $B$.\\
(iii) Find the transverse acceleration of the particle at $B$.

\hfill \mbox{\textit{OCR M3 2013 Q5 [10]}}