Edexcel M2 — Question 7 17 marks

Exam BoardEdexcel
ModuleM2 (Mechanics 2)
Marks17
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicMoments
TypeLadder against wall
DifficultyStandard +0.8 This is a multi-part statics problem requiring resolution of forces, moments about a point, and analysis of limiting equilibrium. While it involves standard M2 techniques (resolving forces, taking moments, finding resultants), the three-part structure with the painter climbing adds complexity. The calculation requires careful handling of the geometry (tan α = 3/4 means sin α = 3/5, cos α = 4/5), and part (c) involves setting up a moment equation with a variable distance. This is more demanding than a routine statics question but doesn't require exceptional insight—it's a solid exam question testing multiple skills in sequence.
Spec3.03m Equilibrium: sum of resolved forces = 03.03n Equilibrium in 2D: particle under forces3.04b Equilibrium: zero resultant moment and force

\includegraphics{figure_7} A uniform ladder \(AB\), of mass \(m\) kg and length \(2a\) m, rests with its upper end \(A\) in contact with a smooth vertical wall and its lower end \(B\) in contact with a fixed peg on horizontal ground. The ladder makes an angle \(\alpha\) with the ground, where \(\tan \alpha = \frac{3}{4}\).
  1. Show that the magnitude of the resultant force acting on the ladder at \(B\) is \(\frac{\sqrt{13}}{3}mg\). [7 marks]
  2. Find, to the nearest degree, the direction of this resultant force at \(B\). [3 marks]
The peg will break when the horizontal force acting on it exceeds \(2mg\) N. A painter of mass \(6m\) kg starts to climb the ladder from \(B\).
  1. Find, in terms of \(a\), the greatest distance up the ladder that the painter can safely climb. [7 marks]

AnswerMarks Guidance
(a) \(R = mg\), \(F = S\)B1 B1 M1 A1
\(M(B): mga \cos \alpha = 2a S \sin \alpha\)M1
\(S = \frac{mg}{2 \tan \alpha} = \frac{2mg}{3}\)A1
\(F = S\)A1
Resultant force at \(B = \sqrt{(mg)^2 + \left(\frac{2mg}{3}\right)^2} = \frac{\sqrt{13}}{3}mg\)M1 A1
(b) Angle \(= \tan^{-1}(3/2) = 56°\) to horizontalM1 A1 A1
(c) \(M(B): mga \cos \alpha + 6mgx \cos \alpha = 2a S \sin \alpha\)M1 A1 A1
\(S = \frac{2mg(a + 6x)}{3a}\)A1 M1 A1
When \(S = 2mg\), \(a + 6x = 3a\)A1 M1 A1
\(6x = 2a\)A1
\(x = \frac{a}{3}\)A1 (17 marks)
(a) $R = mg$, $F = S$ | B1 B1 M1 A1 |

$M(B): mga \cos \alpha = 2a S \sin \alpha$ | M1 |

$S = \frac{mg}{2 \tan \alpha} = \frac{2mg}{3}$ | A1 |

$F = S$ | A1 |

Resultant force at $B = \sqrt{(mg)^2 + \left(\frac{2mg}{3}\right)^2} = \frac{\sqrt{13}}{3}mg$ | M1 A1 |

(b) Angle $= \tan^{-1}(3/2) = 56°$ to horizontal | M1 A1 A1 |

(c) $M(B): mga \cos \alpha + 6mgx \cos \alpha = 2a S \sin \alpha$ | M1 A1 A1 |

$S = \frac{2mg(a + 6x)}{3a}$ | A1 M1 A1 |

When $S = 2mg$, $a + 6x = 3a$ | A1 M1 A1 |

$6x = 2a$ | A1 |

$x = \frac{a}{3}$ | A1 | (17 marks)
\includegraphics{figure_7}

A uniform ladder $AB$, of mass $m$ kg and length $2a$ m, rests with its upper end $A$ in contact with a smooth vertical wall and its lower end $B$ in contact with a fixed peg on horizontal ground. The ladder makes an angle $\alpha$ with the ground, where $\tan \alpha = \frac{3}{4}$.

\begin{enumerate}[label=(\alph*)]
\item Show that the magnitude of the resultant force acting on the ladder at $B$ is $\frac{\sqrt{13}}{3}mg$. [7 marks]
\item Find, to the nearest degree, the direction of this resultant force at $B$. [3 marks]
\end{enumerate}

The peg will break when the horizontal force acting on it exceeds $2mg$ N.

A painter of mass $6m$ kg starts to climb the ladder from $B$.

\begin{enumerate}[label=(\alph*)]
\setcounter{enumi}{2}
\item Find, in terms of $a$, the greatest distance up the ladder that the painter can safely climb. [7 marks]
\end{enumerate}

\hfill \mbox{\textit{Edexcel M2  Q7 [17]}}