| Exam Board | OCR |
|---|---|
| Module | Further Mechanics (Further Mechanics) |
| Year | 2023 |
| Session | June |
| Marks | 13 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Variable Force |
| Type | Variable force (velocity v) - use v dv/dx |
| Difficulty | Challenging +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 neededβmoderately above average difficulty. |
| Spec | 1.08k 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 |
| Answer | Marks | Guidance |
|---|---|---|
| 5 | (a) | 2 v d v = β ( v 2 + 1 ) |
| d x | M1 | 3.3 |
| Answer | Marks |
|---|---|
| only. Allow a single sign error | Condone m seen in equation (not |
| Answer | Marks | Guidance |
|---|---|---|
| v + 1 | M1 | 1.1 |
| Answer | Marks |
|---|---|
| one side | Condone m seen in equation (not |
| Answer | Marks | Guidance |
|---|---|---|
| οln(v2+1)=βx+c | A1 | 1.1 |
| and x (condone missing + c). | Must see brackets for this A mark, |
| Answer | Marks | Guidance |
|---|---|---|
| x = 0 , v = 3 ο c = ln ( u 2 + 1 ) = ln 1 0 | M1 | 3.4 |
| Answer | Marks |
|---|---|
| format ln(π(π£)) = Β±π₯ +π | May see use of limits |
| Answer | Marks | Guidance |
|---|---|---|
| ο v = 1 0 e β x β 1 | A1 | 1.1 |
| Answer | Marks | Guidance |
|---|---|---|
| (b) | v = 2 => ln(22 + 1) = βx + ln10 | M1 |
| Answer | Marks |
|---|---|
| the constant of integration | Or integrating between the correct |
| Answer | Marks | Guidance |
|---|---|---|
| awrt 0.693 m | A1 | 1.1 |
| Answer | Marks | Guidance |
|---|---|---|
| (c) | For Q, F = β1 => a = β0.5 => v = u β 0.5tβ or | |
| v2 = u2 β s | M1 | 1.1 |
| Answer | Marks |
|---|---|
| suvat equation | ALT method 1: (using F = ma to |
| Answer | Marks | Guidance |
|---|---|---|
| v2 = u2 + 2as => s = 9 | A1 | 2.1 |
| Answer | Marks | Guidance |
|---|---|---|
| ο t < 6 and x < 9 | A1 | 2.2a |
| Answer | Marks |
|---|---|
| and x < 9 | Be generous with t and tβ confusion |
| Answer | Marks | Guidance |
|---|---|---|
| (d) | B1 | 3.1b |
| Answer | Marks |
|---|---|
| No values required. | Should come to rest |
| Answer | Marks | Guidance |
|---|---|---|
| (e) | v = 0 => ln1 = βx + ln10 | M1 |
| Answer | Marks |
|---|---|
| form | Or considering 10eβx β 1 β₯ 0 |
| Answer | Marks | Guidance |
|---|---|---|
| or awrt 2.30 m | A1 | 1.1 |
Question 5:
5 | (a) | 2 v d v = β ( 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
ππ₯
2). Do not allow
ππ£
22 v
ο² d v = β 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
οln(v2+1)=βx+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 ο c = ln ( u 2 + 1 ) = ln 1 0 | M1 | 3.4 | Using initial condition to find c
for an expression of correct
format ln(π(π£)) = Β±π₯ +π | May see use of limits
[ln (π£2 +1)]π£ = [βx]π₯
3 0
βln(π£2 +1)βln(10) = βπ₯
ο v 2 + 1 = e β x + c = 1 0 e β x
ο v = 1 0 e β x β 1 | A1 | 1.1 | The β1 must be clearly under the
root sign oe
[5]
(b) | v = 2 => ln(22 + 1) = βx + 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 (π£2 +1)]2 = [βx]π₯
3 0
οln(5)βln(10) = βπ₯
x = ln10 β 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 = β1 => a = β0.5 => v = u β 0.5tβ or
v2 = u2 β 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):
ππ£ ππ£
πΉ = β1 = π = 2
ππ‘ ππ‘
βΉ βπ‘+π = 2π£
At π‘ = 0,π£ = 3 βΉ π = 6
1
Hence π£ = (6βπ‘)
2
ALT method 2:
ππ£
2π£ = β1 βπ£2 = βπ₯ +π
ππ₯
At π₯ = 0,π£ = 3 βπ = 9
Hence π£2 = 9βπ₯ oe
Q stops when v = 0.
Q
v = u + atβ => β0.5tβ = β3 => tβ = 6
v2 = u2 + 2as => s = 9 | A1 | 2.1 | AG Need to see v = 0 used. | ALT method 1
v = 0 when tβ = 6
Q
ππ₯
βπ‘β+6 = 2
ππ‘β
π‘β2
βΉ β +6π‘β(+π) = 2π₯
2
1 π‘β2
(and k = 0) so π₯ = (6π‘ββ )
2 2
At tβ = 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 ο§a ο§ > 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.
ο 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 β 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 tβ 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 = βx + ln10 | M1 | 3.4 | Substituting v = 0 into a solution
of the DE needs to be correct
form | Or considering 10eβx β 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]}}