OCR MEI M3 2006 January — Question 2 18 marks

Exam BoardOCR MEI
ModuleM3 (Mechanics 3)
Year2006
SessionJanuary
Marks18
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicCircular Motion 2
TypeParticle on outer surface of sphere
DifficultyStandard +0.3 This is a standard M3 circular motion question with a particle on a sphere. Part (a) is routine circular motion formula application. Part (b) follows a well-established template: energy conservation to find v², resolving forces radially to show R in terms of θ, finding acceleration components, and determining when R=0 for leaving the surface. All techniques are standard for this topic with no novel insight required, making it slightly easier than average.
Spec6.02d Mechanical energy: KE and PE concepts6.02e Calculate KE and PE: using formulae6.05b Circular motion: v=r*omega and a=v^2/r6.05d Variable speed circles: energy methods6.05e Radial/tangential acceleration

2
  1. A moon of mass \(7.5 \times 10 ^ { 22 } \mathrm {~kg}\) moves round a planet in a circular path of radius \(3.8 \times 10 ^ { 8 } \mathrm {~m}\), completing one orbit in a time of \(2.4 \times 10 ^ { 6 } \mathrm {~s}\). Find the force acting on the moon.
  2. Fig. 2 shows a fixed solid sphere with centre O and radius 4 m . Its surface is smooth. The point A on the surface of the sphere is 3.5 m vertically above the level of O . A particle P of mass 0.2 kg is placed on the surface at A and is released from rest. In the subsequent motion, when OP makes an angle \(\theta\) with the horizontal and P is still on the surface of the sphere, the speed of P is \(v \mathrm {~m} \mathrm {~s} ^ { - 1 }\) and the normal reaction acting on P is \(R \mathrm {~N}\). \begin{figure}[h]
    \includegraphics[alt={},max width=\textwidth]{b7f8bdfd-33dc-4453-8f3a-ddd24be17372-3_746_734_705_662} \captionsetup{labelformat=empty} \caption{Fig. 2}
    \end{figure}
    1. Express \(v ^ { 2 }\) in terms of \(\theta\).
    2. Show that \(R = 5.88 \sin \theta - 3.43\).
    3. Find the radial and tangential components of the acceleration of P when \(\theta = 40 ^ { \circ }\).
    4. Find the value of \(\theta\) at the instant when P leaves the surface of the sphere.

2
\begin{enumerate}[label=(\alph*)]
\item A moon of mass $7.5 \times 10 ^ { 22 } \mathrm {~kg}$ moves round a planet in a circular path of radius $3.8 \times 10 ^ { 8 } \mathrm {~m}$, completing one orbit in a time of $2.4 \times 10 ^ { 6 } \mathrm {~s}$. Find the force acting on the moon.
\item Fig. 2 shows a fixed solid sphere with centre O and radius 4 m . Its surface is smooth. The point A on the surface of the sphere is 3.5 m vertically above the level of O . A particle P of mass 0.2 kg is placed on the surface at A and is released from rest. In the subsequent motion, when OP makes an angle $\theta$ with the horizontal and P is still on the surface of the sphere, the speed of P is $v \mathrm {~m} \mathrm {~s} ^ { - 1 }$ and the normal reaction acting on P is $R \mathrm {~N}$.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{b7f8bdfd-33dc-4453-8f3a-ddd24be17372-3_746_734_705_662}
\captionsetup{labelformat=empty}
\caption{Fig. 2}
\end{center}
\end{figure}
\begin{enumerate}[label=(\roman*)]
\item Express $v ^ { 2 }$ in terms of $\theta$.
\item Show that $R = 5.88 \sin \theta - 3.43$.
\item Find the radial and tangential components of the acceleration of P when $\theta = 40 ^ { \circ }$.
\item Find the value of $\theta$ at the instant when P leaves the surface of the sphere.
\end{enumerate}\end{enumerate}

\hfill \mbox{\textit{OCR MEI M3 2006 Q2 [18]}}