Edexcel M3 2016 January — Question 1 6 marks

Exam BoardEdexcel
ModuleM3 (Mechanics 3)
Year2016
SessionJanuary
Marks6
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicCircular Motion 1
TypeParticle in hemispherical bowl
DifficultyStandard +0.3 This is a standard M3 circular motion problem requiring resolution of forces (normal reaction and weight) and application of F=mrω². The geometry is straightforward (30-60-90 triangle gives angle), and the method is routine for this topic. Slightly easier than average due to being a 'show that' question with clear target and standard technique.
Spec6.05c Horizontal circles: conical pendulum, banked tracks

1. \begin{figure}[h]
\includegraphics[alt={},max width=\textwidth]{ffe0bc72-3136-48d9-9d5b-4a364d134070-02_503_524_121_712} \captionsetup{labelformat=empty} \caption{Figure 1}
\end{figure} A hemispherical bowl of internal radius \(2 r\) is fixed with its circular rim horizontal. A particle \(P\) is moving in a horizontal circle of radius \(r\) on the smooth inner surface of the bowl, as shown in Figure 1. Particle \(P\) is moving with constant angular speed \(\omega\). Show that \(\omega = \sqrt { \frac { g \sqrt { 3 } } { 3 r } }\)

Question 1:
AnswerMarks Guidance
Answer/WorkingMarks Guidance
\(R\sin 60° = mg\)M1A1 Resolve vertically, allow with \(60°\) or \(\theta\); correct equation with \(60°\) or \(\theta\)
\(R\cos 60° = mr\omega^2\)M1A1 Equation of motion along radius, acceleration in either form, \(60°\) or \(\theta\); correct equation with \(60°\) or \(\theta\), acceleration to be \(r\omega^2\)
\(\tan 60° = \dfrac{g}{r\omega^2}\)ddM1 Eliminate \(R\), substitute numerical value for \(\theta\) and solve to \(\omega = \ldots\) or \(\omega^2 = \ldots\); depends on both previous M marks
\(\omega = \sqrt{\dfrac{g}{r\sqrt{3}}} = \sqrt{\dfrac{g\sqrt{3}}{3r}}\)A1cso Complete to the given answer
**Question 1:**

| Answer/Working | Marks | Guidance |
|---|---|---|
| $R\sin 60° = mg$ | M1A1 | Resolve vertically, allow with $60°$ or $\theta$; correct equation with $60°$ or $\theta$ |
| $R\cos 60° = mr\omega^2$ | M1A1 | Equation of motion along radius, acceleration in either form, $60°$ or $\theta$; correct equation with $60°$ or $\theta$, acceleration to be $r\omega^2$ |
| $\tan 60° = \dfrac{g}{r\omega^2}$ | ddM1 | Eliminate $R$, substitute numerical value for $\theta$ and solve to $\omega = \ldots$ or $\omega^2 = \ldots$; depends on both previous M marks |
| $\omega = \sqrt{\dfrac{g}{r\sqrt{3}}} = \sqrt{\dfrac{g\sqrt{3}}{3r}}$ | A1cso | Complete to the given answer |
1.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{ffe0bc72-3136-48d9-9d5b-4a364d134070-02_503_524_121_712}
\captionsetup{labelformat=empty}
\caption{Figure 1}
\end{center}
\end{figure}

A hemispherical bowl of internal radius $2 r$ is fixed with its circular rim horizontal. A particle $P$ is moving in a horizontal circle of radius $r$ on the smooth inner surface of the bowl, as shown in Figure 1. Particle $P$ is moving with constant angular speed $\omega$.

Show that $\omega = \sqrt { \frac { g \sqrt { 3 } } { 3 r } }$\\

\hfill \mbox{\textit{Edexcel M3 2016 Q1 [6]}}