| Exam Board | OCR |
|---|---|
| Module | H240/03 (Pure Mathematics and Mechanics) |
| Year | 2019 |
| Session | June |
| Marks | 14 |
| Paper | Download PDF ↗ |
| Topic | Moments |
| Type | Ladder against wall |
| Difficulty | Standard +0.3 This is a standard A-level mechanics ladder problem requiring moments about a point, resolving forces, and using limiting friction. Part (a) is routine moment calculation, part (b) applies friction law, part (c) is simple algebra, and part (d) is recall. The problem follows a well-established template with clear scaffolding and no novel insight required. |
| Spec | 1.05c Area of triangle: using 1/2 ab sin(C) |
\begin{tikzpicture}[scale=1.2, thick]
% Compute positions
\pgfmathsetmacro{\Wx}{2*3.5*cos(30)}
\pgfmathsetmacro{\By}{2*3.5*sin(30)}
\coordinate (A) at (0,0);
\coordinate (W) at (\Wx,0);
\coordinate (B) at (\Wx,\By);
\coordinate (C) at ({0.35*\Wx},{0.35*\By});
\coordinate (midAB) at ({0.5*\Wx},{0.5*\By});
\coordinate (midAC) at ({0.175*\Wx},{0.175*\By});
% Ground
\draw (-.5,0) -- ({\Wx+1},0);
\foreach \x in {-0.3,0.0,...,6.3} {
\draw (\x,0) -- ++(-.2,-.2);
}
% Wall
\fill[gray!60] (\Wx,0) rectangle ++(0.15,{\By+0.8});
\draw (\Wx,0) -- (\Wx,{\By+0.8});
% Ladder
\draw (A) -- (B);
% Angle arc at A
\draw (0.9,0) arc[start angle=0, end angle=30, radius=0.9];
\node at (1.15,0.22) {$30^\circ$};
% Height h label
\draw[<->] ({\Wx+0.6},0) -- ({\Wx+0.6},\By);
\node[right] at ({\Wx+0.6},{0.5*\By}) {$h$};
% Label 2a along ladder
\node[above left] at (midAB) {$2a$};
% Label d from A to C
\node[above left] at (midAC) {$d$};
% Point C dot and label
\fill (C) circle (2pt);
\node[below right] at (C) {$C$};
% Labels for A and B
\node[below left] at (A) {$A$};
\node[right] at (B) {$B$};
\end{tikzpicture}
The diagram shows a ladder $AB$, of length $2a$ and mass $m$, resting in equilibrium on a vertical wall of height $h$. The ladder is inclined at an angle of $30°$ to the horizontal. The end $A$ is in contact with horizontal ground. An object of mass $2m$ is placed on the ladder at a point $C$ where $AC = d$.
The ladder is modelled as uniform, the ground is modelled as being rough, and the vertical wall is modelled as being smooth.
\begin{enumerate}[label=(\alph*)]
\item Show that the normal contact force between the ladder and the wall is $\frac{mg(a + 2d)\sqrt{3}}{4h}$. [4]
\end{enumerate}
It is given that the equilibrium is limiting and the coefficient of friction between the ladder and the ground is $\frac{1}{3}\sqrt{3}$.
\begin{enumerate}[label=(\alph*)]
\setcounter{enumii}{1}
\item Show that $h = k(a + 2d)$, where $k$ is a constant to be determined. [7]
\item Hence find, in terms of $a$, the greatest possible value of $d$. [2]
\item State one improvement that could be made to the model. [1]
\end{enumerate}
\hfill \mbox{\textit{OCR H240/03 2019 Q11 [14]}}