Edexcel FM1 2022 June — Question 6 13 marks

Exam BoardEdexcel
ModuleFM1 (Further Mechanics 1)
Year2022
SessionJune
Marks13
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicAdvanced work-energy problems
TypeConnected particles pulley energy method
DifficultyStandard +0.3 This is a standard Further Mechanics 1 connected particles problem using work-energy principles. Part (a) requires straightforward PE calculations with sin θ = 3/5 from tan θ = 3/4. Part (b) applies work-energy to find friction coefficient—routine for FM1. Part (c) requires careful consideration of motion after B hits ground, but follows standard work-energy methodology. The multi-part structure and trigonometry add some complexity, but all techniques are standard FM1 fare with no novel insights required.
Spec3.03v Motion on rough surface: including inclined planes6.02i Conservation of energy: mechanical energy principle6.02j Conservation with elastics: springs and strings

6. \begin{figure}[h]
\includegraphics[alt={},max width=\textwidth]{86a37170-046f-46e5-9c8c-06d5f98ca4fe-20_497_1337_246_365} \captionsetup{labelformat=empty} \caption{Figure 4}
\end{figure} Two blocks, \(A\) and \(B\), of masses 2 kg and 4 kg respectively are attached to the ends of a light inextensible string. Initially \(A\) is held on a fixed rough plane. The plane is inclined to horizontal ground at an angle \(\theta\), where \(\tan \theta = \frac { 3 } { 4 }\) The string passes over a small smooth light pulley \(P\) that is fixed at the top of the plane. The part of the string from \(A\) to \(P\) is parallel to a line of greatest slope of the plane. Block \(A\) is held on the plane with the distance \(A P\) greater than 3 m .
Block \(B\) hangs freely below \(P\) at a distance of 3 m above the ground, as shown in Figure 4. The coefficient of friction between \(A\) and the plane is \(\mu\) Block \(A\) is released from rest with the string taut.
By modelling the blocks as particles,
  1. find the potential energy lost by the whole system as a result of \(B\) falling 3 m . Given that the speed of \(B\) at the instant it hits the ground is \(4.5 \mathrm {~m} \mathrm {~s} ^ { - 1 }\) and ignoring air resistance,
  2. use the work-energy principle to find the value of \(\mu\) After \(B\) hits the ground, \(A\) continues to move up the plane but does not reach the pulley in the subsequent motion.
    Block \(A\) comes to instantaneous rest after moving a total distance of ( \(3 + d\) ) m from its point of release. Ignoring air resistance,
  3. use the work-energy principle to find the value of \(d\) \includegraphics[max width=\textwidth, alt={}, center]{86a37170-046f-46e5-9c8c-06d5f98ca4fe-20_2255_50_309_1981}

Question 6:
Part 6(a):
AnswerMarks Guidance
Answer/WorkingMark Guidance
GPE lost by \(B\) – GPE gained by \(A\)M1 Expression for change in GPE. Must be dimensionally correct and resolved terms where necessary. Allow subtraction either way round
\(= 4 \times g \times 3 - 2 \times g \sin\theta \times 3\)A1 Correct unsimplified expression for change in PE (before substitution for \(\sin\theta\)). Allow subtraction either way round
\(= 82\ (82.3)\) (J)A1 2 sf or 3 sf. Accept \(8.4g\) or \(\frac{42g}{5}\). Must be positive but condone a sign change at end without explanation
(3 marks)
Part 6(b):
AnswerMarks Guidance
Answer/WorkingMark Guidance
Total KE gained \(= \frac{1}{2} \times 6 \times 4.5^2\ (= 60.75)\) (J)B1 Gain in KE for the system (not just one block)
Max friction \(\mu 2g\cos\theta\ (= \mu \times 2 \times 9.8 \times \cos\theta = 15.68\mu)\)B1 Correct unsimplified expression for \(F_{\max}\) seen or implied
Work done against friction \(= 3 \times F_{\max}\ (= 47.04\mu)\)B1ft Correct expression for work done; follow their \(F_{\max}\). Dependent on having found \(F_{\max}\)
Work-energy equation: their GPE lost = their KE gained + their WD against frictionM1 Complete method using work-energy to form equation in \(\mu\). Require all terms (KE and GPE of both blocks). Dimensionally correct. Condone sign errors
\(82.32 = 60.75 + 47.04\mu\)A1 Correct unsimplified equation in \(\mu\)
\(\mu = 0.459\ (0.46)\)A1 3 sf or 2 sf only
(6 marks)
> NB: Alternative via tension in string: B1 for KE of \(B\) and correct tension (25.7 N); B1 for \(F_{\max}\); B1ft for work done by tension and against friction; M1 for \(3 \times 25.7 = 20.25 + 35.28 + 3 \times 15.68\mu\)
Part 6(c):
AnswerMarks Guidance
Answer/WorkingMark Guidance
Work-energy equation for \(A\)M1 All terms required. Dimensionally correct. Condone sign errors and \(\sin/\cos\) confusion. If equation uses \(d+3\) in place of \(d\) in PE term, correct only if also includes term for initial PE. If \(d+3\) used in work done term, scores M0
\(\frac{1}{2} \times 2 \times 4.5^2 = 2g\sin\theta \times d + 2g\cos\theta \times \mu d\) \(\left(= 19.6 \times \frac{3}{5} \times d + 19.6 \times \frac{4}{5} \times \mu d\right)\)A1ft Unsimplified equation in \(d\) and \(\mu\) with at most one error
A1ftCorrect unsimplified equation in \(d\) and \(\mu\). ft is on their \(\mu\) if substituted
\(d = 1.07\ (1.1)\)A1 3 sf or 2 sf only
(4 marks)
## Question 6:

### Part 6(a):

| Answer/Working | Mark | Guidance |
|---|---|---|
| GPE lost by $B$ – GPE gained by $A$ | M1 | Expression for change in GPE. Must be dimensionally correct and resolved terms where necessary. Allow subtraction either way round |
| $= 4 \times g \times 3 - 2 \times g \sin\theta \times 3$ | A1 | Correct unsimplified expression for change in PE (before substitution for $\sin\theta$). Allow subtraction either way round |
| $= 82\ (82.3)$ (J) | A1 | 2 sf or 3 sf. Accept $8.4g$ or $\frac{42g}{5}$. Must be positive but condone a sign change at end without explanation |

**(3 marks)**

---

### Part 6(b):

| Answer/Working | Mark | Guidance |
|---|---|---|
| Total KE gained $= \frac{1}{2} \times 6 \times 4.5^2\ (= 60.75)$ (J) | B1 | Gain in KE for the system (not just one block) |
| Max friction $\mu 2g\cos\theta\ (= \mu \times 2 \times 9.8 \times \cos\theta = 15.68\mu)$ | B1 | Correct unsimplified expression for $F_{\max}$ seen or implied |
| Work done against friction $= 3 \times F_{\max}\ (= 47.04\mu)$ | B1ft | Correct expression for work done; follow their $F_{\max}$. Dependent on having found $F_{\max}$ |
| Work-energy equation: their GPE lost = their KE gained + their WD against friction | M1 | Complete method using work-energy to form equation in $\mu$. Require all terms (KE and GPE of both blocks). Dimensionally correct. Condone sign errors |
| $82.32 = 60.75 + 47.04\mu$ | A1 | Correct unsimplified equation in $\mu$ |
| $\mu = 0.459\ (0.46)$ | A1 | 3 sf or 2 sf only |

**(6 marks)**

> **NB:** Alternative via tension in string: B1 for KE of $B$ and correct tension (25.7 N); B1 for $F_{\max}$; B1ft for work done by tension and against friction; M1 for $3 \times 25.7 = 20.25 + 35.28 + 3 \times 15.68\mu$

---

### Part 6(c):

| Answer/Working | Mark | Guidance |
|---|---|---|
| Work-energy equation for $A$ | M1 | All terms required. Dimensionally correct. Condone sign errors and $\sin/\cos$ confusion. If equation uses $d+3$ in place of $d$ in PE term, correct only if also includes term for initial PE. If $d+3$ used in work done term, scores M0 |
| $\frac{1}{2} \times 2 \times 4.5^2 = 2g\sin\theta \times d + 2g\cos\theta \times \mu d$ $\left(= 19.6 \times \frac{3}{5} \times d + 19.6 \times \frac{4}{5} \times \mu d\right)$ | A1ft | Unsimplified equation in $d$ and $\mu$ with at most one error |
| | A1ft | Correct unsimplified equation in $d$ and $\mu$. ft is on their $\mu$ if substituted |
| $d = 1.07\ (1.1)$ | A1 | 3 sf or 2 sf only |

**(4 marks)**

---
6.

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{86a37170-046f-46e5-9c8c-06d5f98ca4fe-20_497_1337_246_365}
\captionsetup{labelformat=empty}
\caption{Figure 4}
\end{center}
\end{figure}

Two blocks, $A$ and $B$, of masses 2 kg and 4 kg respectively are attached to the ends of a light inextensible string.

Initially $A$ is held on a fixed rough plane. The plane is inclined to horizontal ground at an angle $\theta$, where $\tan \theta = \frac { 3 } { 4 }$\\
The string passes over a small smooth light pulley $P$ that is fixed at the top of the plane. The part of the string from $A$ to $P$ is parallel to a line of greatest slope of the plane.

Block $A$ is held on the plane with the distance $A P$ greater than 3 m .\\
Block $B$ hangs freely below $P$ at a distance of 3 m above the ground, as shown in Figure 4.

The coefficient of friction between $A$ and the plane is $\mu$\\
Block $A$ is released from rest with the string taut.\\
By modelling the blocks as particles,
\begin{enumerate}[label=(\alph*)]
\item find the potential energy lost by the whole system as a result of $B$ falling 3 m .

Given that the speed of $B$ at the instant it hits the ground is $4.5 \mathrm {~m} \mathrm {~s} ^ { - 1 }$ and ignoring air resistance,
\item use the work-energy principle to find the value of $\mu$

After $B$ hits the ground, $A$ continues to move up the plane but does not reach the pulley in the subsequent motion.\\
Block $A$ comes to instantaneous rest after moving a total distance of ( $3 + d$ ) m from its point of release.

Ignoring air resistance,
\item use the work-energy principle to find the value of $d$\\
\includegraphics[max width=\textwidth, alt={}, center]{86a37170-046f-46e5-9c8c-06d5f98ca4fe-20_2255_50_309_1981}
\end{enumerate}

\hfill \mbox{\textit{Edexcel FM1 2022 Q6 [13]}}