Pre-U Pre-U 9794/3 2014 June — Question 9 7 marks

Exam BoardPre-U
ModulePre-U 9794/3 (Pre-U Mathematics Paper 3)
Year2014
SessionJune
Marks7
TopicMotion on a slope
TypeMotion down rough slope
DifficultyModerate -0.3 This is a standard mechanics problem on inclined planes with friction. Part (i) is routine diagram drawing, part (ii) requires resolving forces and applying F=ma (standard A-level technique with 5 marks suggesting straightforward working), and part (iii) tests conceptual understanding of the friction condition. While it requires multiple steps, it follows a well-established method with no novel insight needed, making it slightly easier than average.
Spec3.03a Force: vector nature and diagrams3.03r Friction: concept and vector form3.03v Motion on rough surface: including inclined planes

A particle of mass \(m\) is placed on a rough inclined plane. The plane makes an angle \(\theta\) with the horizontal. The coefficient of friction between the particle and the plane is \(\mu\) where \(\mu < \tan \theta\). The particle is released from rest and accelerates down the plane.
  1. Draw a fully labelled diagram to show the forces acting on the particle. [1]
  2. Find an expression in terms of \(g\), \(\theta\) and \(\mu\) for the acceleration of the particle. [5]
  3. Explain what would happen to the particle if \(\mu > \tan \theta\). [1]

AnswerMarks Guidance
(i) Diagram showing weight, normal contact force and friction, and no othersB1 [1]
(ii) Resolve perpendicular to slope:B1 M1 Equation of motion with 3 terms, and at least 2 correct. Condone consistent sin/cos error.
\(N2L\) used & resolve down slope:
\(N = mg \cos \theta\)
\(ma = mg \sin \theta - F\)
Friction law:B1 Limiting friction only.
\(F = \mu N\)M1 Attempt to eliminate \(N\) and \(F\), and cancel \(m\).
\(\therefore ma = mg \sin \theta - \mu mg \cos \theta\)
\(\therefore a = g(\sin \theta - \mu \cos \theta)\)A1 c.a.o. [5]
(iii) If \(\mu > \tan \theta\) then the particle will not move.B1 [1]
**(i)** Diagram showing weight, normal contact force and friction, and no others | B1 | [1]

**(ii)** Resolve perpendicular to slope: | B1 M1 | Equation of motion with 3 terms, and at least 2 correct. Condone consistent sin/cos error.

$N2L$ used & resolve down slope: | 

$N = mg \cos \theta$ | 

$ma = mg \sin \theta - F$ | 

Friction law: | B1 | Limiting friction only.

$F = \mu N$ | M1 | Attempt to eliminate $N$ and $F$, and cancel $m$.

$\therefore ma = mg \sin \theta - \mu mg \cos \theta$ | 

$\therefore a = g(\sin \theta - \mu \cos \theta)$ | A1 | c.a.o. [5]

**(iii)** If $\mu > \tan \theta$ then the particle will not move. | B1 | [1]
A particle of mass $m$ is placed on a rough inclined plane. The plane makes an angle $\theta$ with the horizontal. The coefficient of friction between the particle and the plane is $\mu$ where $\mu < \tan \theta$. The particle is released from rest and accelerates down the plane.

\begin{enumerate}[label=(\roman*)]
\item Draw a fully labelled diagram to show the forces acting on the particle. [1]
\item Find an expression in terms of $g$, $\theta$ and $\mu$ for the acceleration of the particle. [5]
\item Explain what would happen to the particle if $\mu > \tan \theta$. [1]
\end{enumerate}

\hfill \mbox{\textit{Pre-U Pre-U 9794/3 2014 Q9 [7]}}