| Exam Board | OCR MEI |
|---|---|
| Module | Further Mechanics Major (Further Mechanics Major) |
| Year | 2024 |
| Session | June |
| Marks | 16 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Circular Motion 2 |
| Type | Projectile motion after leaving circle |
| Difficulty | Challenging +1.2 This is a multi-part circular motion and projectile problem requiring energy methods, Newton's second law in circular motion, and projectile analysis. While it involves several steps and techniques (tangential acceleration, tension calculation using energy conservation and circular motion equations, projectile motion after string breaks), each individual part follows standard Further Maths mechanics procedures without requiring novel insight. The 'show that' parts provide target values, reducing problem-solving demand. Slightly above average difficulty due to the multi-stage nature and need to coordinate multiple mechanics concepts. |
| Spec | 3.02h Motion under gravity: vector form3.02i Projectile motion: constant acceleration model6.05e Radial/tangential acceleration6.05f Vertical circle: motion including free fall |
| Answer | Marks |
|---|---|
| 11(a) | 1×gcos20=1×a |
| a=9.21 (m s−2) | M1 |
| Answer | Marks |
|---|---|
| [2] | 3.3 |
| 1.1 | Use of F = ma tangentially soi – allow without explicitly |
| Answer | Marks |
|---|---|
| 11(b) | 1×v2 |
| Answer | Marks |
|---|---|
| θ=23.1 | M1* |
| Answer | Marks |
|---|---|
| [5] | 3.3 |
| Answer | Marks |
|---|---|
| 1.1 | Use of N2L radially – correct number of terms – allow |
| Answer | Marks |
|---|---|
| 11(c) | Vertical distance to fall is 1.55 or 1.75−0.5sin23.1 |
| Answer | Marks |
|---|---|
| V =6.67(m s-1) | B1 |
| Answer | Marks |
|---|---|
| [4] | 3.1b |
| Answer | Marks |
|---|---|
| 1.1 | Allow 1523or an answer in the interval [1.544, 1.554] – |
| Answer | Marks |
|---|---|
| M1 | Conservation of Energy (loss of PE = gain in KE) – |
| Answer | Marks | Guidance |
|---|---|---|
| 2 | A1 A1 | A1 for correct LHS, A1 for correct RHS |
| v=6.67(m s-1) | A1 | awrt 6.67 – 3 sf or better |
| Answer | Marks |
|---|---|
| 11(d) | 1.75−0.5sin23.1=(3.75cos23.1)t+0.5gt2 |
| Answer | Marks |
|---|---|
| almost directly below O) | M1* |
| Answer | Marks |
|---|---|
| [5] | 3.3 |
| Answer | Marks |
|---|---|
| 3.5a | For vertical motion – if correct expect to see |
Question 11:
--- 11(a) ---
11(a) | 1×gcos20=1×a
a=9.21 (m s−2) | M1
A1
[2] | 3.3
1.1 | Use of F = ma tangentially soi – allow without explicitly
seeing m = 1 and award this mark for m×gcos20=m×a-
condone sign errors and sin/cos mix only
awrt 9.21or allow 9.2 www
--- 11(b) ---
11(b) | 1×v2
32−1×gsinθ=
0.5
1(1)(3.2)2 = 1(1)v2 −1(g)(0.5sinθ)
2 2
Substitute for v2 in energy equation
1(1)(3.2)2 = 1(1)(16−0.5×1×gsinθ)−1(g)(0.5sinθ)
2 2
θ=23.1 | M1*
M1*
M1dep*
A1
A1
[5] | 3.3
1.1
3.4
1.1
1.1 | Use of N2L radially – correct number of terms – allow
sign errors and sin/cos mix - allow without explicitly
seeing m = 1 stated/used– must be using a= mv2 with
r
correct values of m and r but allow T for 32 for this mark
Use of conservation of energy (correct number of terms
with h=0.5sinθ or h=0.5cosθ only (if taking the initial
position as PE = 0)) – allow sign errors
Or solve simultaneous equations in v2 and sinθ (oe) – all
values must have been substituted for this mark
Correct equation in θ only – note that
32=29.4sinθ+20.48(oe) scores the first four marks
AG allow awrt 23.1 (for reference: 23.068…) should be
from sinθ= 96 or 0.3918… - condone 23.1 being stated
245
after a correct equation (as AG must check this
carefully) – any wrong working seen scores A0 – note
that θmight be defined as the angle to the vertical – if
90−θis then considered then allow for full marks
--- 11(c) ---
11(c) | Vertical distance to fall is 1.55 or 1.75−0.5sin23.1
Velocity when string breaks is 3.75 (m s-1)
1V2 = 1×3.752 +g(1.75−0.5sin23.1)or
2 2
V2 =(3.75×sin23.1)2 +(3.75×cos23.1)2 +2×g×1.55
V =6.67(m s-1) | B1
B1
M1
A1
[4] | 3.1b
1.1
3.4
1.1 | Allow 1523or an answer in the interval [1.544, 1.554] –
980
3 sf (e.g. 1.54 or 1.55) or better
Allow for v2 = 352 or v= 4 22 or awrt 3.75 for v or a
25 5
value in the interval [14.077, 14.085] for v2– 3 sf (e.g.
3.75) or better (allow un-simplified e.g.
v= 10.24+gsin23.1 or v= 16−0.5×gsin23.1)
Conservation of Energy with correct number of terms but
allow sign errors – with their 14.08 or 3.75 (but M0 if
using 3.2) – for h allow from 1.75−0.5sin23.1 or
1.75−0.5cos23.1 only. Their 3.75 must come from an
equation with the correct number of relevant terms. If
using v2 =u2 +2as to find V, then must be using the
equivalent of their 3.75 and not just a single component
of their 3.75 (must also be using a=±g )
If using exact values may see V2 = 2227 - awrt 6.67 – 3 sf
50
or better
Alternative solution
M1 | Conservation of Energy (loss of PE = gain in KE) –
setting up an equation with the correct number of terms
using the 1.75, 3.2 and the speed of P at A only
1×g×1.75= 1×1×(v2 −3.22)
2 | A1 A1 | A1 for correct LHS, A1 for correct RHS
v=6.67(m s-1) | A1 | awrt 6.67 – 3 sf or better
--- 11(d) ---
11(d) | 1.75−0.5sin23.1=(3.75cos23.1)t+0.5gt2
Time to A is 0.312 (s)
Horizontal distance travelled = 0.31...×(3.75sin23.1)
Distance = 0.459
(Which is very close to) 0.5cos23.1=0.460(so A is
almost directly below O) | M1*
A1
M1dep*
A1
A1
[5] | 3.3
1.1
3.4
1.1
3.5a | For vertical motion – if correct expect to see
1.55...=3.45t+0.5gt2 - using their 3.75 ×cos23.1 or
their 3.75 ×sin23.1(from part (c)). Allow sign errors on
RHS, but LHS must be 1.75−0.5sin23.1only. Must be
using a=±g.
Watch out for other complete methods that lead to the
time of flight e.g. finding the two vertical components of
velocity and applying v=u+atwith a= g e.g. if correct
expect to see 6.51−3.45= gtor 6.50−3.45= gt (oe)
awrt 0.312 or awrt 0.311 or allow 0.31 www (if using exact
then answer is 0.3121…) – also allow correct un-
6.51(or 6.50)−3.45
simplified expression for t e.g. (but
g
must be a correct expression for t and not just an equation
containing t)
Use of s = ut horizontally with their t – allow sin/cos mix
but must be using the correct value of 3.75 now
awrt 0.459 or 0.458 www (but not just 0.46) – so must
have been using a correct t
Must either explicitly state that 0.5cos23.1 = 0.459… or
0.46 (or better) or show the difference between the two
values is very close to zero (if either value is not
explicitly stated) – as a minimum must show explicitly
both values (but no further comment required) www
(dependent on all previous marks)
A particle P of mass 1 kg is fixed to one end of a light inextensible string of length 0.5 m. The other end of the string is attached to a fixed point O, which is 1.75 m above a horizontal plane. P is held with the string horizontal and taut. P is then projected vertically downwards with a speed of $3.2 \text{ m s}^{-1}$.
\begin{enumerate}[label=(\alph*)]
\item Find the tangential acceleration of P when OP makes an angle of $20°$ with the horizontal. [2]
\end{enumerate}
The string breaks when the tension in it is 32 N. At this point the angle between OP and the horizontal is $\theta$.
\begin{enumerate}[label=(\alph*)]
\setcounter{enumi}{1}
\item Show that $\theta = 23.1°$, correct to 1 decimal place. [5]
\end{enumerate}
Particle P subsequently hits the plane at a point A.
\begin{enumerate}[label=(\alph*)]
\setcounter{enumi}{2}
\item Determine the speed of P when it arrives at A. [4]
\item Show that A is almost vertically below O. [5]
\end{enumerate}
\hfill \mbox{\textit{OCR MEI Further Mechanics Major 2024 Q11 [16]}}