AQA Paper 2 Specimen — Question 12 4 marks

Exam BoardAQA
ModulePaper 2 (Paper 2)
SessionSpecimen
Marks4
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicTravel graphs
TypeFind acceleration from SUVAT
DifficultyModerate -0.8 This is a straightforward derivation of standard SUVAT equations from first principles using basic algebra and gradient interpretation. Part (a) requires simple gradient calculation (1 mark), and part (b) is a guided algebraic manipulation with clear steps provided by the given displacement formula. This is easier than average as it's purely mechanical algebra with no problem-solving insight required.
Spec3.02b Kinematic graphs: displacement-time and velocity-time3.02c Interpret kinematic graphs: gradient and area3.02d Constant acceleration: SUVAT formulae

A particle moves on a straight line with a constant acceleration, \(a\) m s\(^{-2}\). The initial velocity of the particle is \(U\) m s\(^{-1}\). After \(T\) seconds the particle has velocity \(V\) m s\(^{-1}\). This information is shown on the velocity-time graph. \includegraphics{figure_12} The displacement, \(S\) metres, of the particle from its initial position at time \(T\) seconds is given by the formula $$S = \frac{1}{2}(U + V)T$$
  1. By considering the gradient of the graph, or otherwise, write down a formula for \(a\) in terms of \(U\), \(V\) and \(T\). [1 mark]
  2. Hence show that \(V^2 = U^2 + 2aS\) [3 marks]

Question 12:

AnswerMarks Guidance
12(a)States correct expression for a AO1.1b
a
T
AnswerMarks Guidance
(b)Rearranges to make T the subject
of the formulaAO2.1 R1
T 
a
1 V U
S  (U V)
2 a
2as (U V)(V U)
V2 U2 2aS (AG)
Uses given expression for S and
AnswerMarks Guidance
attempts to eliminate TAO2.1 R1
Completes argument to reach
required result AG
Only award if they have a
completely correct solution, which
is clear, easy to follow and
AnswerMarks Guidance
contains no slipsAO2.1 R1
Total4
QMarking Instructions AO
Question 12:
--- 12(a) ---
12(a) | States correct expression for a | AO1.1b | B1 | V U
a
T
(b) | Rearranges to make T the subject
of the formula | AO2.1 | R1 | V U
T 
a
1 V U
S  (U V)
2 a
2as (U V)(V U)
V2 U2 2aS (AG)
Uses given expression for S and
attempts to eliminate T | AO2.1 | R1
Completes argument to reach
required result AG
Only award if they have a
completely correct solution, which
is clear, easy to follow and
contains no slips | AO2.1 | R1
Total | 4
Q | Marking Instructions | AO | Marks | Typical Solution
A particle moves on a straight line with a constant acceleration, $a$ m s$^{-2}$.

The initial velocity of the particle is $U$ m s$^{-1}$.

After $T$ seconds the particle has velocity $V$ m s$^{-1}$.

This information is shown on the velocity-time graph.

\includegraphics{figure_12}

The displacement, $S$ metres, of the particle from its initial position at time $T$ seconds is given by the formula
$$S = \frac{1}{2}(U + V)T$$

\begin{enumerate}[label=(\alph*)]
\item By considering the gradient of the graph, or otherwise, write down a formula for $a$ in terms of $U$, $V$ and $T$.
[1 mark]

\item Hence show that $V^2 = U^2 + 2aS$
[3 marks]
\end{enumerate}

\hfill \mbox{\textit{AQA Paper 2  Q12 [4]}}