OCR Further Mechanics 2023 June — Question 5 13 marks

Exam BoardOCR
ModuleFurther Mechanics (Further Mechanics)
Year2023
SessionJune
Marks13
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicVariable Force
TypeVariable force (velocity v) - use v dv/dx
DifficultyChallenging +1.3 This is a Further Mechanics question requiring Newton's second law with variable resistance, separation of variables, and integration. Parts (a)-(b) are standard technique (F=ma leading to v dv/dx = -Β½(vΒ²+1), then integrate), part (c) requires comparative reasoning about forces, and part (e) needs finding when v=0. While multi-step and requiring several techniques, the methods are all standard for Further Mechanics with no novel insights neededβ€”moderately above average difficulty.
Spec1.08k Separable differential equations: dy/dx = f(x)g(y)3.03b Newton's first law: equilibrium6.06a Variable force: dv/dt or v*dv/dx methods

A particle \(P\) of mass \(2\) kg moves along the \(x\)-axis. At time \(t = 0\), \(P\) passes through the origin \(O\) with speed \(3\) m s\(^{-1}\). At time \(t\) seconds the displacement of \(P\) from \(O\) is \(x\) m and the velocity of \(P\) is \(v\) m s\(^{-1}\), where \(t \geqslant 0\), \(x \geqslant 0\) and \(v \geqslant 0\). While \(P\) is in motion the only force acting on \(P\) is a resistive force \(F\) of magnitude \((v^2 + 1)\) N acting in the negative \(x\)-direction.
  1. Find an expression for \(v\) in terms of \(x\). [5]
  2. Determine the distance travelled by \(P\) while its speed drops from \(3\) m s\(^{-1}\) to \(2\) m s\(^{-1}\). [2]
Particle \(Q\) is identical to particle \(P\). At a different time, \(Q\) is moving along the \(x\)-axis under the influence of a single constant resistive force of magnitude \(1\) N. When \(t' = 0\), \(Q\) is at the origin and its speed is \(3\) m s\(^{-1}\).
  1. By comparing the motion of \(P\) with the motion of \(Q\) explain why \(P\) must come to rest at some finite time when \(t < 6\) with \(x < 9\). [3]
  2. Sketch the velocity-time graph for \(P\). You do not need to indicate any values on your sketch. [1]
  3. Determine the maximum displacement of \(P\) from \(O\) during \(P\)'s motion. [2]

Question 5:
AnswerMarks Guidance
5(a) 2 v d v = βˆ’ ( v 2 + 1 )
d xM1 3.3
differential equation in v and x
AnswerMarks
only. Allow a single sign errorCondone m seen in equation (not
𝑑π‘₯
2). Do not allow
𝑑𝑣
22 v
 d v = βˆ’ x + c
AnswerMarks Guidance
v + 1M1 1.1
variables and integrating at least
AnswerMarks
one sideCondone m seen in equation (not
2). Can be given if m substituted
later
AnswerMarks Guidance
ln(v2+1)=βˆ’x+cA1 1.1
and x (condone missing + c).Must see brackets for this A mark,
and correct numerical m.
AnswerMarks Guidance
x = 0 , v = 3 οƒž c = ln ( u 2 + 1 ) = ln 1 0M1 3.4
for an expression of correct
AnswerMarks
format ln(𝑓(𝑣)) = Β±π‘₯ +𝑐May see use of limits
[ln (𝑣2 +1)]𝑣 = [βˆ’x]π‘₯
3 0
β‡’ln(𝑣2 +1)βˆ’ln(10) = βˆ’π‘₯
 v 2 + 1 = e βˆ’ x + c = 1 0 e βˆ’ x
AnswerMarks Guidance
 v = 1 0 e βˆ’ x βˆ’ 1A1 1.1
root sign oe
[5]
AnswerMarks Guidance
(b)v = 2 => ln(22 + 1) = –x + ln10 M1
of the correct form, which
includes a numerical value for
AnswerMarks
the constant of integrationOr integrating between the correct
limits.
[ln (𝑣2 +1)]2 = [βˆ’x]π‘₯
3 0
οƒžln(5)βˆ’ln(10) = βˆ’π‘₯
x = ln10 – ln5 = ln2 so distance is ln2 m or
AnswerMarks Guidance
awrt 0.693 mA1 1.1
working (need to see v=2)
[2]
AnswerMarks Guidance
(c)For Q, F = –1 => a = –0.5 => v = u – 0.5t’ or
v2 = u2 – sM1 1.1
acceleration and using it in a
AnswerMarks
suvat equationALT method 1: (using F = ma to
set up a differential equation):
𝑑𝑣 𝑑𝑣
𝐹 = βˆ’1 = π‘š = 2
𝑑𝑑 𝑑𝑑
⟹ βˆ’π‘‘+𝑐 = 2𝑣
At 𝑑 = 0,𝑣 = 3 ⟹ 𝑐 = 6
1
Hence 𝑣 = (6βˆ’π‘‘)
2
ALT method 2:
𝑑𝑣
2𝑣 = βˆ’1 ⇒𝑣2 = βˆ’π‘₯ +𝑐
𝑑π‘₯
At π‘₯ = 0,𝑣 = 3 ⇒𝑐 = 9
Hence 𝑣2 = 9βˆ’π‘₯ oe
Q stops when v = 0.
Q
v = u + at’ => –0.5t’ = –3 => t’ = 6
AnswerMarks Guidance
v2 = u2 + 2as => s = 9A1 2.1
v = 0 when t’ = 6
Q
𝑑π‘₯
βˆ’π‘‘β€™+6 = 2
𝑑𝑑’
𝑑’2
⟹ βˆ’ +6𝑑’(+π‘˜) = 2π‘₯
2
1 𝑑’2
(and k = 0) so π‘₯ = (6π‘‘β€™βˆ’ )
2 2
At t’ = 6, x = 9
ALT method 2
Q stops when v=0, therefore 9-x =
0, therefore x = 9.
They will also need to use one of
the other listed methods to justify
the limit on t for this method mark
But for P, F = 1 + v2 > 1 (so a  > 0.5 for all
P
v) so P will slow down more quickly than Q
(and be travelling more slowly at any
comparable time) so it must stop before time
t = 6 and it cannot reach x = 9.
AnswerMarks Guidance
 t < 6 and x < 9A1 2.2a
β€’ F = 1 + v2 > 1 (explicit
comparison)
β€’ A reference to P coming
to rest more quickly than
Q (comparison). Needs
to make the link – a
larger resistive force will
decelerate P more
quickly or a larger
resistive force will mean
P is travelling more
slowly than Q (from
starting point of 3)
β€’ Final conclusion: So it
comes to rest when t < 6
AnswerMarks
and x < 9Be generous with t and t’ confusion
[3]
AnswerMarks Guidance
(d)B1 3.1b
Strictly decreasing from positive
value on vertical (v) axis to the
horizontal (t) axis. Negative
gradient at vertical axis
intercept. Allow concave. Do
not allow linear
AnswerMarks
No values required.Should come to rest
[1]
AnswerMarks Guidance
(e)v = 0 => ln1 = –x + ln10 M1
of the DE needs to be correct
AnswerMarks
formOr considering 10e–x – 1 β‰₯ 0
x = ln10 so maximum displacement is ln10 m
AnswerMarks Guidance
or awrt 2.30 mA1 1.1
working (need to see v=0)
[2]
Question 5:
5 | (a) | 2 v d v = βˆ’ ( v 2 + 1 )
d x | M1 | 3.3 | Using F = ma to derive a
differential equation in v and x
only. Allow a single sign error | Condone m seen in equation (not
𝑑π‘₯
2). Do not allow
𝑑𝑣
22 v
 d v = βˆ’ x + c
v + 1 | M1 | 1.1 | Correctly separating the
variables and integrating at least
one side | Condone m seen in equation (not
2). Can be given if m substituted
later
ln(v2+1)=βˆ’x+c | A1 | 1.1 | Correct relationship between v
and x (condone missing + c). | Must see brackets for this A mark,
and correct numerical m.
x = 0 , v = 3 οƒž c = ln ( u 2 + 1 ) = ln 1 0 | M1 | 3.4 | Using initial condition to find c
for an expression of correct
format ln(𝑓(𝑣)) = Β±π‘₯ +𝑐 | May see use of limits
[ln (𝑣2 +1)]𝑣 = [βˆ’x]π‘₯
3 0
β‡’ln(𝑣2 +1)βˆ’ln(10) = βˆ’π‘₯
 v 2 + 1 = e βˆ’ x + c = 1 0 e βˆ’ x
 v = 1 0 e βˆ’ x βˆ’ 1 | A1 | 1.1 | The –1 must be clearly under the
root sign oe
[5]
(b) | v = 2 => ln(22 + 1) = –x + ln10 | M1 | 3.4 | Substituting v = 2 into a solution
of the correct form, which
includes a numerical value for
the constant of integration | Or integrating between the correct
limits.
[ln (𝑣2 +1)]2 = [βˆ’x]π‘₯
3 0
οƒžln(5)βˆ’ln(10) = βˆ’π‘₯
x = ln10 – ln5 = ln2 so distance is ln2 m or
awrt 0.693 m | A1 | 1.1 | Award SC1 if answer seen with no
working (need to see v=2)
[2]
(c) | For Q, F = –1 => a = –0.5 => v = u – 0.5t’ or
v2 = u2 – s | M1 | 1.1 | Calculating the (constant)
acceleration and using it in a
suvat equation | ALT method 1: (using F = ma to
set up a differential equation):
𝑑𝑣 𝑑𝑣
𝐹 = βˆ’1 = π‘š = 2
𝑑𝑑 𝑑𝑑
⟹ βˆ’π‘‘+𝑐 = 2𝑣
At 𝑑 = 0,𝑣 = 3 ⟹ 𝑐 = 6
1
Hence 𝑣 = (6βˆ’π‘‘)
2
ALT method 2:
𝑑𝑣
2𝑣 = βˆ’1 ⇒𝑣2 = βˆ’π‘₯ +𝑐
𝑑π‘₯
At π‘₯ = 0,𝑣 = 3 ⇒𝑐 = 9
Hence 𝑣2 = 9βˆ’π‘₯ oe
Q stops when v = 0.
Q
v = u + at’ => –0.5t’ = –3 => t’ = 6
v2 = u2 + 2as => s = 9 | A1 | 2.1 | AG Need to see v = 0 used. | ALT method 1
v = 0 when t’ = 6
Q
𝑑π‘₯
βˆ’π‘‘β€™+6 = 2
𝑑𝑑’
𝑑’2
⟹ βˆ’ +6𝑑’(+π‘˜) = 2π‘₯
2
1 𝑑’2
(and k = 0) so π‘₯ = (6π‘‘β€™βˆ’ )
2 2
At t’ = 6, x = 9
ALT method 2
Q stops when v=0, therefore 9-x =
0, therefore x = 9.
They will also need to use one of
the other listed methods to justify
the limit on t for this method mark
But for P, F = 1 + v2 > 1 (so a  > 0.5 for all
P
v) so P will slow down more quickly than Q
(and be travelling more slowly at any
comparable time) so it must stop before time
t = 6 and it cannot reach x = 9.
 t < 6 and x < 9 | A1 | 2.2a | AG Include:
β€’ F = 1 + v2 > 1 (explicit
comparison)
β€’ A reference to P coming
to rest more quickly than
Q (comparison). Needs
to make the link – a
larger resistive force will
decelerate P more
quickly or a larger
resistive force will mean
P is travelling more
slowly than Q (from
starting point of 3)
β€’ Final conclusion: So it
comes to rest when t < 6
and x < 9 | Be generous with t and t’ confusion
[3]
(d) | B1 | 3.1b | Graph in 1st quadrant only.
Strictly decreasing from positive
value on vertical (v) axis to the
horizontal (t) axis. Negative
gradient at vertical axis
intercept. Allow concave. Do
not allow linear
No values required. | Should come to rest
[1]
(e) | v = 0 => ln1 = –x + ln10 | M1 | 3.4 | Substituting v = 0 into a solution
of the DE needs to be correct
form | Or considering 10e–x – 1 β‰₯ 0
x = ln10 so maximum displacement is ln10 m
or awrt 2.30 m | A1 | 1.1 | Allow -ln(1/10) | Award SC1 if answer seen with no
working (need to see v=0)
[2]
A particle $P$ of mass $2$ kg moves along the $x$-axis.

At time $t = 0$, $P$ passes through the origin $O$ with speed $3$ m s$^{-1}$.

At time $t$ seconds the displacement of $P$ from $O$ is $x$ m and the velocity of $P$ is $v$ m s$^{-1}$, where $t \geqslant 0$, $x \geqslant 0$ and $v \geqslant 0$.

While $P$ is in motion the only force acting on $P$ is a resistive force $F$ of magnitude $(v^2 + 1)$ N acting in the negative $x$-direction.

\begin{enumerate}[label=(\alph*)]
\item Find an expression for $v$ in terms of $x$. [5]
\item Determine the distance travelled by $P$ while its speed drops from $3$ m s$^{-1}$ to $2$ m s$^{-1}$. [2]
\end{enumerate}

Particle $Q$ is identical to particle $P$. At a different time, $Q$ is moving along the $x$-axis under the influence of a single constant resistive force of magnitude $1$ N. When $t' = 0$, $Q$ is at the origin and its speed is $3$ m s$^{-1}$.

\begin{enumerate}[label=(\alph*)]
\setcounter{enumi}{2}
\item By comparing the motion of $P$ with the motion of $Q$ explain why $P$ must come to rest at some finite time when $t < 6$ with $x < 9$. [3]
\item Sketch the velocity-time graph for $P$. You do not need to indicate any values on your sketch. [1]
\item Determine the maximum displacement of $P$ from $O$ during $P$'s motion. [2]
\end{enumerate}

\hfill \mbox{\textit{OCR Further Mechanics 2023 Q5 [13]}}