SPS SPS ASFM 2020 May — Question 8 14 marks

Exam BoardSPS
ModuleSPS ASFM (SPS ASFM)
Year2020
SessionMay
Marks14
TopicPulley systems
TypeThree or more connected particles
DifficultyStandard +0.3 This is a standard circular motion problem with connected particles requiring force resolution, geometry to find angles (3-4-5 triangle), and energy calculations. While multi-part with several steps, each component uses routine A-level mechanics techniques without requiring novel insight or particularly challenging problem-solving.
Spec6.02i Conservation of energy: mechanical energy principle6.04e Rigid body equilibrium: coplanar forces

\includegraphics{figure_8} As shown in the diagram, \(AB\) is a long thin rod which is fixed vertically with \(A\) above \(B\). One end of a light inextensible string of length 1 m is attached to \(A\) and the other end is attached to a particle \(P\) of mass \(m_1\) kg. One end of another light inextensible string of length 1 m is also attached to \(P\). Its other end is attached to a small smooth ring \(R\), of mass \(m_2\) kg, which is free to move on \(AB\). Initially, \(P\) moves in a horizontal circle of radius 0.6 m with constant angular velocity \(\omega \mathrm{rad s}^{-1}\). The magnitude of the tension in string \(AP\) is denoted by \(T_1\) N while that in string \(PR\) is denoted by \(T_2\) N.
  1. By considering forces on \(R\), express \(T_2\) in terms of \(m_2\). [2]
  2. Show that
    1. \(T_1 = \frac{49}{4}(m_1 + m_2)\), [2]
    2. \(\omega^2 = \frac{49(m_1 + 2m_2)}{4m_1}\). [3]
  3. Deduce that, in the case where \(m_1\) is much bigger than \(m_2\), \(\omega \approx 3.5\). [2] In a different case, where \(m_1 = 2.5\) and \(m_2 = 2.8\), \(P\) slows down. Eventually the system comes to rest with \(P\) and \(R\) hanging in equilibrium.
  4. Find the total energy lost by \(P\) and \(R\) as the angular velocity of \(P\) changes from the initial value of \(\omega \mathrm{rad s}^{-1}\) to zero. [5]

\includegraphics{figure_8}

As shown in the diagram, $AB$ is a long thin rod which is fixed vertically with $A$ above $B$. One end of a light inextensible string of length 1 m is attached to $A$ and the other end is attached to a particle $P$ of mass $m_1$ kg. One end of another light inextensible string of length 1 m is also attached to $P$. Its other end is attached to a small smooth ring $R$, of mass $m_2$ kg, which is free to move on $AB$.

Initially, $P$ moves in a horizontal circle of radius 0.6 m with constant angular velocity $\omega \mathrm{rad s}^{-1}$. The magnitude of the tension in string $AP$ is denoted by $T_1$ N while that in string $PR$ is denoted by $T_2$ N.

\begin{enumerate}[label=(\alph*)]
\item By considering forces on $R$, express $T_2$ in terms of $m_2$. [2]

\item Show that
\begin{enumerate}[label=(\roman*)]
\item $T_1 = \frac{49}{4}(m_1 + m_2)$, [2]
\item $\omega^2 = \frac{49(m_1 + 2m_2)}{4m_1}$. [3]
\end{enumerate}

\item Deduce that, in the case where $m_1$ is much bigger than $m_2$, $\omega \approx 3.5$. [2]

In a different case, where $m_1 = 2.5$ and $m_2 = 2.8$, $P$ slows down. Eventually the system comes to rest with $P$ and $R$ hanging in equilibrium.

\item Find the total energy lost by $P$ and $R$ as the angular velocity of $P$ changes from the initial value of $\omega \mathrm{rad s}^{-1}$ to zero. [5]
\end{enumerate}

\hfill \mbox{\textit{SPS SPS ASFM 2020 Q8 [14]}}