Edexcel M1 — Question 5 12 marks

Exam BoardEdexcel
ModuleM1 (Mechanics 1)
Marks12
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicFriction
TypeSingle angled force - find limiting friction or coefficient
DifficultyStandard +0.3 This is a standard M1 friction problem requiring resolution of forces and application of F=μR. Part (a) is routine 'show that' with given answer; part (b) applies F=ma after finding resultant force. Both parts follow textbook methods with no novel problem-solving required, making it slightly easier than average.
Spec3.03c Newton's second law: F=ma one dimension3.03e Resolve forces: two dimensions3.03t Coefficient of friction: F <= mu*R model3.03u Static equilibrium: on rough surfaces

\includegraphics{figure_2} Figure 2 shows a large block of mass 50 kg being pulled on rough horizontal ground by means of a rope attached to the block. The tension in the rope is 200 N and it makes an angle of 40° with the horizontal. Under these conditions, the block is on the point of moving. Modelling the block as a particle,
  1. show that the coefficient of friction between the block and the ground is 0.424 correct to 3 significant figures. [6 marks]
The angle with the horizontal at which the rope is being pulled is reduced to 30°. Ignoring air resistance and assuming that the tension in the rope and the coefficient of friction remain unchanged,
  1. find the acceleration of the block. [6 marks]

AnswerMarks Guidance
(a) resolve \(\uparrow\): \(R + 200\sin40° - 50g = 0 \therefore R = 50g - 200\sin40°\) resolve \(\rightarrow\): \(200\cos40° - F = 0 \therefore F = 200\cos40°\) \(F = \mu R\), so \(\mu = \frac{200\cos40°}{50g - 200\sin40°} = 0.424\) (3sf)M1 A1 M1 A1 M1 A1
(b) resolve \(\uparrow\): \(R + 200\sin30° - 50g = 0 \therefore R = 50g - 200\sin30° = 390\) resolve \(\rightarrow\): \(200\cos30° - \mu R = 50a\) \(50a = 100\sqrt{3} - 0.424(390)\) \(a = 0.16 \text{ ms}^{-2}\)M1 A1 M1 A1 M1 A1 (12)
**(a)** resolve $\uparrow$: $R + 200\sin40° - 50g = 0 \therefore R = 50g - 200\sin40°$ resolve $\rightarrow$: $200\cos40° - F = 0 \therefore F = 200\cos40°$ $F = \mu R$, so $\mu = \frac{200\cos40°}{50g - 200\sin40°} = 0.424$ (3sf) | M1 A1 M1 A1 M1 A1 |

**(b)** resolve $\uparrow$: $R + 200\sin30° - 50g = 0 \therefore R = 50g - 200\sin30° = 390$ resolve $\rightarrow$: $200\cos30° - \mu R = 50a$ $50a = 100\sqrt{3} - 0.424(390)$ $a = 0.16 \text{ ms}^{-2}$ | M1 A1 M1 A1 M1 A1 | (12)

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\includegraphics{figure_2}

Figure 2 shows a large block of mass 50 kg being pulled on rough horizontal ground by means of a rope attached to the block. The tension in the rope is 200 N and it makes an angle of 40° with the horizontal. Under these conditions, the block is on the point of moving.

Modelling the block as a particle,

\begin{enumerate}[label=(\alph*)]
\item show that the coefficient of friction between the block and the ground is 0.424 correct to 3 significant figures. [6 marks]
\end{enumerate}

The angle with the horizontal at which the rope is being pulled is reduced to 30°. Ignoring air resistance and assuming that the tension in the rope and the coefficient of friction remain unchanged,

\begin{enumerate}[label=(\alph*)]\setcounter{enumi}{1}
\item find the acceleration of the block. [6 marks]
\end{enumerate}

\hfill \mbox{\textit{Edexcel M1  Q5 [12]}}