Edexcel FM2 AS 2024 June — Question 3 11 marks

Exam BoardEdexcel
ModuleFM2 AS (Further Mechanics 2 AS)
Year2024
SessionJune
Marks11
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicVariable acceleration (1D)
TypeAcceleration as function of velocity (separation of variables)
DifficultyStandard +0.3 This is a standard Further Maths variable acceleration question requiring separation of variables and integration with initial conditions. The differential equation a = dv/dt = 4 - 3v is straightforward to separate and integrate, and part (b) requires a second integration. While it's FM content, it follows a well-established template with no conceptual surprises, making it slightly easier than average overall.
Spec1.08d Evaluate definite integrals: between limits1.08k Separable differential equations: dy/dx = f(x)g(y)3.02f Non-uniform acceleration: using differentiation and integration

  1. A particle \(P\) is moving along the \(x\)-axis. At time \(t\) seconds, \(P\) has velocity \(v \mathrm {~m} \mathrm {~s} ^ { - 1 }\) in the positive \(x\) direction and acceleration \(a \mathrm {~ms} ^ { - 2 }\) in the positive \(x\) direction.
In a model of the motion of \(P\) $$a = 4 - 3 v$$ When \(t = 0 , v = 0\)
  1. Use integration to show that \(v = k \left( 1 - \mathrm { e } ^ { - 3 t } \right)\), where \(k\) is a constant to be found. When \(t = 0 , P\) is at the origin \(O\)
  2. Find, in terms of \(t\) only, the distance of \(P\) from \(O\) at time \(t\) seconds.

3a
AnswerMarks Guidance
\(a = 4 - 3v \Rightarrow \int \frac{1}{4-3v}dv = \int 1dt\)M1 2.1
Integrate both sides of the equationM1 1.1b
\(\Rightarrow -\frac{1}{3}\ln\4-3v\ = t(+C)\)
Use \(t=0, v=0\)M1 3.4
\(t = \frac{1}{3}\ln\left(\frac{4}{4-3v}\right)\)A1 1.1b
\(\Rightarrow e^{3t} = \frac{4}{4-3v}, \quad 4-3v = 4e^{-3t}\)M1 1.1b
\(v = \frac{4}{3}\left(1 - e^{-3t}\right)\) *A1* 2.2a
(7)
3b
AnswerMarks Guidance
\(\frac{dx}{dt} = k\left(1 - e^{-3t}\right) \Rightarrow \int 1dx = \int k\left(1 - e^{-3t}\right)dt\)M1 3.3
\(x = k\left(t + \frac{1}{3}e^{-3t}\right)(+C) = \frac{4}{3}\left(t + \frac{1}{3}e^{-3t}\right)(+C)\)M1 1.1b
Use \(t=0, x=0\)M1 3.4
\(x = k\left(t + \frac{1}{3}e^{-3t} - \frac{1}{3}\right) = \frac{4}{3}\left(t + \frac{1}{3}e^{-3t} - \frac{1}{3}\right)\)A1ft 1.1b
(4)
(11 marks)
Notes for 3a:
- M1: Use \(a = \frac{dv}{dt}\) and separate the variables to form integrals in \(v\) and \(t\)
- M1: Integrate to obtain terms \(p\ln(4-3v)\) and \(qt\)
- A1: Or equivalent. Accept with brackets in place of modulus signs. Condone missing constant of integration
- M1: Use boundary conditions in the model to evaluate constant of integration or as limits on a definite integral
- A1: Or equivalent
- M1: Rearrange to obtain expression for \(v\) in terms of \(t\)
- A1*: Obtain given form with \(k = \frac{4}{3}\) from correct working
Notes for 3b:
- M1: Use \(v = \frac{dx}{dt}\) to form integrals in \(x\) and \(t\)
- M1: Integrate to obtain \(\lambda t + \mu e^{-3t}(+C)\)
- M1: Use boundary conditions in the model to evaluate constant of integration or as limits on a definite integral
- A1 ft: Any equivalent form. Follow their \(k\)
**3a**

| $a = 4 - 3v \Rightarrow \int \frac{1}{4-3v}dv = \int 1dt$ | M1 | 2.1 |
| Integrate both sides of the equation | M1 | 1.1b |
| $\Rightarrow -\frac{1}{3}\ln\|4-3v\| = t(+C)$ | A1 | 1.1b |
| Use $t=0, v=0$ | M1 | 3.4 |
| $t = \frac{1}{3}\ln\left(\frac{4}{4-3v}\right)$ | A1 | 1.1b |
| $\Rightarrow e^{3t} = \frac{4}{4-3v}, \quad 4-3v = 4e^{-3t}$ | M1 | 1.1b |
| $v = \frac{4}{3}\left(1 - e^{-3t}\right)$ * | A1* | 2.2a |
| | (7) | |

**3b**

| $\frac{dx}{dt} = k\left(1 - e^{-3t}\right) \Rightarrow \int 1dx = \int k\left(1 - e^{-3t}\right)dt$ | M1 | 3.3 |
| $x = k\left(t + \frac{1}{3}e^{-3t}\right)(+C) = \frac{4}{3}\left(t + \frac{1}{3}e^{-3t}\right)(+C)$ | M1 | 1.1b |
| Use $t=0, x=0$ | M1 | 3.4 |
| $x = k\left(t + \frac{1}{3}e^{-3t} - \frac{1}{3}\right) = \frac{4}{3}\left(t + \frac{1}{3}e^{-3t} - \frac{1}{3}\right)$ | A1ft | 1.1b |
| | (4) | |
| | (11 marks) | |

**Notes for 3a:**
- M1: Use $a = \frac{dv}{dt}$ and separate the variables to form integrals in $v$ and $t$
- M1: Integrate to obtain terms $p\ln(4-3v)$ and $qt$
- A1: Or equivalent. Accept with brackets in place of modulus signs. Condone missing constant of integration
- M1: Use boundary conditions in the model to evaluate constant of integration or as limits on a definite integral
- A1: Or equivalent
- M1: Rearrange to obtain expression for $v$ in terms of $t$
- A1*: Obtain given form with $k = \frac{4}{3}$ from correct working

**Notes for 3b:**
- M1: Use $v = \frac{dx}{dt}$ to form integrals in $x$ and $t$
- M1: Integrate to obtain $\lambda t + \mu e^{-3t}(+C)$
- M1: Use boundary conditions in the model to evaluate constant of integration or as limits on a definite integral
- A1 ft: Any equivalent form. Follow their $k$

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\begin{enumerate}
  \item A particle $P$ is moving along the $x$-axis. At time $t$ seconds, $P$ has velocity $v \mathrm {~m} \mathrm {~s} ^ { - 1 }$ in the positive $x$ direction and acceleration $a \mathrm {~ms} ^ { - 2 }$ in the positive $x$ direction.
\end{enumerate}

In a model of the motion of $P$

$$a = 4 - 3 v$$

When $t = 0 , v = 0$\\
(a) Use integration to show that $v = k \left( 1 - \mathrm { e } ^ { - 3 t } \right)$, where $k$ is a constant to be found.

When $t = 0 , P$ is at the origin $O$\\
(b) Find, in terms of $t$ only, the distance of $P$ from $O$ at time $t$ seconds.

\hfill \mbox{\textit{Edexcel FM2 AS 2024 Q3 [11]}}