OCR MEI M1 2006 January — Question 7 16 marks

Exam BoardOCR MEI
ModuleM1 (Mechanics 1)
Year2006
SessionJanuary
Marks16
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicFriction
TypePractical friction scenarios
DifficultyModerate -0.3 This is a multi-part mechanics question involving friction and forces, but each part follows standard procedures: resolving forces horizontally/vertically, applying F=ma, and using kinematic equations. While it has 6 parts spanning 13 marks, none require novel insight—just systematic application of M1 techniques. Slightly easier than average due to straightforward setup and clear progression through parts.
Spec3.03c Newton's second law: F=ma one dimension3.03u Static equilibrium: on rough surfaces3.03v Motion on rough surface: including inclined planes

7 Clive and Ken are trying to move a box of mass 50 kg on a rough, horizontal floor. As shown in Fig. 7, Clive always pushes horizontally and Ken always pulls at an angle of \(30 ^ { \circ }\) to the horizontal. Each of them applies forces to the box in the same vertical plane as described below. \begin{figure}[h]
\includegraphics[alt={},max width=\textwidth]{19d42df9-e752-4d33-85e1-4ec59b32135a-4_360_745_995_660} \captionsetup{labelformat=empty} \caption{Fig. 7}
\end{figure} Initially, the box is in equilibrium with Clive pushing with a force of 60 N and Ken not pulling at all.
  1. What is the resistance to motion of the box? Ken now adds a pull of 70 N to Clive's push of 60 N . The box remains in equilibrium.
  2. What now is the resistance to motion of the box?
  3. Calculate the normal reaction of the floor on the box. The frictional resistance to sliding of the box is 125 N .
    Clive now pushes with a force of 160 N but Ken does not pull at all.
  4. Calculate the acceleration of the box. Clive stops pushing when the box has a speed of \(1.5 \mathrm {~m} \mathrm {~s} ^ { - 1 }\).
  5. How far does the box then slide before coming to rest? Ken and Clive now try again. Ken pulls with a force of \(Q \mathrm {~N}\) and Clive pushes with a force of 160 N . The frictional resistance to sliding of the box is now 115 N and the acceleration of the box is \(3 \mathrm {~m} \mathrm {~s} ^ { - 2 }\).
  6. Calculate the value of \(Q\).

7 Clive and Ken are trying to move a box of mass 50 kg on a rough, horizontal floor. As shown in Fig. 7, Clive always pushes horizontally and Ken always pulls at an angle of $30 ^ { \circ }$ to the horizontal. Each of them applies forces to the box in the same vertical plane as described below.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{19d42df9-e752-4d33-85e1-4ec59b32135a-4_360_745_995_660}
\captionsetup{labelformat=empty}
\caption{Fig. 7}
\end{center}
\end{figure}

Initially, the box is in equilibrium with Clive pushing with a force of 60 N and Ken not pulling at all.\\
(i) What is the resistance to motion of the box?

Ken now adds a pull of 70 N to Clive's push of 60 N . The box remains in equilibrium.\\
(ii) What now is the resistance to motion of the box?\\
(iii) Calculate the normal reaction of the floor on the box.

The frictional resistance to sliding of the box is 125 N .\\
Clive now pushes with a force of 160 N but Ken does not pull at all.\\
(iv) Calculate the acceleration of the box.

Clive stops pushing when the box has a speed of $1.5 \mathrm {~m} \mathrm {~s} ^ { - 1 }$.\\
(v) How far does the box then slide before coming to rest?

Ken and Clive now try again. Ken pulls with a force of $Q \mathrm {~N}$ and Clive pushes with a force of 160 N . The frictional resistance to sliding of the box is now 115 N and the acceleration of the box is $3 \mathrm {~m} \mathrm {~s} ^ { - 2 }$.\\
(vi) Calculate the value of $Q$.

\hfill \mbox{\textit{OCR MEI M1 2006 Q7 [16]}}