| Exam Board | OCR MEI |
|---|---|
| Module | Further Mechanics Major (Further Mechanics Major) |
| Year | 2024 |
| Session | June |
| Marks | 10 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Circular Motion 1 |
| Type | Particle on cone surface – with string attached to vertex or fixed point |
| Difficulty | Challenging +1.8 This is a challenging 3D mechanics problem requiring resolution of forces in multiple directions, circular motion dynamics, and constraint analysis. Part (a) demands careful geometric reasoning to relate string length, radius of circular motion, and depth h, then combining tension equations from both particles. Part (b) requires understanding that loss of contact occurs when normal reaction becomes zero. The multi-step algebraic manipulation and 3D visualization elevate this significantly above routine mechanics questions, though the techniques themselves are standard for Further Mechanics. |
| Spec | 6.05c Horizontal circles: conical pendulum, banked tracks6.05e Radial/tangential acceleration |
| Answer | Marks |
|---|---|
| 13(a) | T =4g |
| Answer | Marks |
|---|---|
| ⇒4hsin2α+5cos2α=10cosα | B1* |
| Answer | Marks |
|---|---|
| [7] | 1.1 |
| Answer | Marks |
|---|---|
| 2.1 | Resolving vertically for P (soi e.g. in an equation for Q) |
| Answer | Marks | Guidance |
|---|---|---|
| T =4g | B1 | Resolving vertically for P (soi) |
| Answer | Marks | Guidance |
|---|---|---|
| 2r(2.8)2sinα | B1 | soi – allow any trigonometric expression containing h and |
| Answer | Marks | Guidance |
|---|---|---|
| T −2gcosα=2(htanα)(2.8)2sinα | M1 | Applying N2L parallel to the slope for Q – correct |
| Answer | Marks | Guidance |
|---|---|---|
| 4g−2gcosα=2(htanα)(2.8)2sinα | A3 | Award A2 for all terms correct but with sign errors only, |
| Answer | Marks |
|---|---|
| ⇒4hsin2α+5cos2α=10cosα | A1 |
| Answer | Marks |
|---|---|
| 13(b) | 4gcosα=2g or 4gsinα=2(htanα)(2.8)2 |
| Answer | Marks |
|---|---|
| 4 | M1* |
| Answer | Marks |
|---|---|
| [3] | 3.1b |
| Answer | Marks |
|---|---|
| 2.2a | Setting R=0 or R>0or R0 in either their |
| Answer | Marks |
|---|---|
| Response | Mark |
Question 13:
--- 13(a) ---
13(a) | T =4g
Tcosα+Rsinα=2g
4gcosα+Rsinα=2g
Tsinα−Rcosα=2(htanα)(2.8)2
4gsinα−Rcosα=2(htanα)(2.8)2
2g−4gcosα
4gsinα−cosα =15.68htanα
sinα
4cosα−2cos2α=1.6hsin2α
⇒4hsin2α+5cos2α=10cosα | B1*
M1*
A1
M1*
A1
M1dep*
A1
[7] | 1.1
3.3
1.1
3.3
1.1
3.4
2.1 | Resolving vertically for P (soi e.g. in an equation for Q)
Attempt to resolve vertically for Q – correct number of
relevant terms so must contain a component of T and R
but allow sign errors and sin/cos mix, must be
dimensionally consistent and using correct mass of 2 kg
but allow T instead of 4g
Where R is the normal contact force between Q and the
surface of the shell – must be using 4g for T now
Applying N2L radially for Q – correct number of
relevant terms so must contain a component of T and R
but allow sign errors and sin/cos mix on LHS, must be
dimensionally consistent and using correct mass of 2 kg
but allow T instead of 4g – must be using a=r(2.8)2with
h
eitherr =htanαor r = only (may have sub. for R)
tanα
oe e.g. 4gsinα−Rcosα=15.68htanα – must be using
4g for T now – note that substituting an incorrect
expression for R can still imply this mark
Eliminate R from the two equations to obtain an equation
in h and αonly
e.g. k =4,k =5 and k =10 (must be integers but accept
1 2 3
multiples of these but must be in this form) – values of k
do not need to be stated explicitly
Alternative Solution – applying N2L parallel to
the surface of the shell
T =4g | B1 | Resolving vertically for P (soi)
Acceleration component parallel to the plane is
2r(2.8)2sinα | B1 | soi – allow any trigonometric expression containing h and
αfor r but not just r
T −2gcosα=2(htanα)(2.8)2sinα | M1 | Applying N2L parallel to the slope for Q – correct
number of relevant terms (allow sign errors and sin/cos
mix on LHS), must be dimensionally consistent (so
component of Q’s mass but no component with T) and
using correct mass of 2 kg but allow T instead of 4g. Must
be using a=r(2.8)2sinα or a=r(2.8)2cosαwith either
h
r =htanαor r = only – if no component of
tanα
acceleration used then M0
4g−2gcosα=2(htanα)(2.8)2sinα | A3 | Award A2 for all terms correct but with sign errors only,
and A1 for sign errors only with a =(htanα)(2.8)2cosα
4gcosα−2gcos2α=15.68hsin2α
⇒4hsin2α+5cos2α=10cosα | A1
e.g. k =4,k =5 and k =10 (must be integers but accept
1 2 3
multiples of these but must be in this form) – values of k
do not need to be stated explicitly
[7]
Acceleration component parallel to the plane is
2r(2.8)2sinα
B1
αfor r but not just r
Applying N2L parallel to the slope for Q – correct
number of relevant terms (allow sign errors and sin/cos
mix on LHS), must be dimensionally consistent (so
component of Q’s mass but no component with T) and
using correct mass of 2 kg but allow T instead of 4g. Must
be using a=r(2.8)2sinα or a=r(2.8)2cosαwith either
h
r =htanαor r = only – if no component of
tanα
acceleration used then M0
T −2gcosα=2(htanα)(2.8)2sinα
M1
4gcosα−2gcos2α=15.68hsin2α
⇒4hsin2α+5cos2α=10cosα
A1
--- 13(b) ---
13(b) | 4gcosα=2g or 4gsinα=2(htanα)(2.8)2
e.g.
cosα= 1 ⇒4g× 3 =2h× 3×2.82or
2 2
cosα= 1 ⇒4h×3+5×1 =10×1
2 4 4 2
h= 5
4 | M1*
M1dep*
A1
[3] | 3.1b
2.1
2.2a | Setting R=0 or R>0or R0 in either their
4gcosα+Rsinα=2g or their
4gsinα−Rcosα=2(htanα)(2.8)2equation to obtain an
equation/inequality in α(and possibly h) only –
dependent on having scored the corresponding M
mark in part (a) or full working in this part (e.g. if
applying N2L parallel to the surface only in part (a))
Substituting their 4gcosα=2ginto either their
4gsinα=2(htanα)(2.8)2or their answer to part (a) oe
correct method that leads to an equation/inequality in h
only - dependent on having scored the corresponding
M mark(s) in part (a) or full working in this part
If h 5 or h< 5then must explicitly state that the
4 4
greatest value is 5 www
4
Response | Mark
The first three marks are for forming two equations that can be used to find both F and R - most candidates will resolve
A A
horizontally and vertically to the rod (see main scheme). However, they may resolve parallel and perpendicular to the rod or take
moments again. There are two marks for the first equation (M1 A1) and one mark (A1) for the second. Please mark to the benefit of
the candidate so one correct equation and one incorrect equation would score 2 out of 3. The same rule applies for the second M
mark in that their equations must contain the required number of relevant terms (so if they take moments again about a different
point and e.g. a force/distance is missing then M0 for the second M mark).
1.5 1.5 1.5
M(peg): −2 ×3gcos25+ ×F sin25= ×R cos25
sin25 sin25 A sin25 A
1.5
M(com): −2 ×R +2×F sin25=2×R cos25
sin25 P A A
1.5
M(B):4− ×R +4×R cos25=2×3gcos25+4×F sin25
sin25 P A A
R(parallel): F cos25+R sin25=3gsin25
A A
R(perpendicular): R+R cos25= F sin25+3gcos25
A A
PMT
Need to get in touch?
If you ever have any questions about OCR qualifications or services (including administration, logistics and teaching) please feel free to get in
touch with our customer support centre.
Call us on
01223 553998
Alternatively, you can email us on
support@ocr.org.uk
For more information visit
ocr.org.uk/qualifications/resource-finder
ocr.org.uk
Twitter/ocrexams
/ocrexams
/company/ocr
/ocrexams
OCR is part of Cambridge University Press & Assessment, a department of the University of Cambridge.
For staff training purposes and as part of our quality assurance programme your call may be recorded or monitored. © OCR
2024 Oxford Cambridge and RSA Examinations is a Company Limited by Guarantee. Registered in England. Registered office
The Triangle Building, Shaftesbury Road, Cambridge, CB2 8EA.
Registered company number 3484466. OCR is an exempt charity.
OCR operates academic and vocational qualifications regulated by Ofqual, Qualifications Wales and CCEA as listed in their
qualifications registers including A Levels, GCSEs, Cambridge Technicals and Cambridge Nationals.
OCR provides resources to help you deliver our qualifications. These resources do not represent any particular teaching method
we expect you to use. We update our resources regularly and aim to make sure content is accurate but please check the OCR
website so that you have the most up-to-date version. OCR cannot be held responsible for any errors or omissions in these
resources.
Though we make every effort to check our resources, there may be contradictions between published support and the
specification, so it is important that you always use information in the latest specification. We indicate any specification changes
within the document itself, change the version number and provide a summary of the changes. If you do notice a discrepancy
between the specification and a resource, please contact us.
Whether you already offer OCR qualifications, are new to OCR or are thinking about switching, you can request more
information using our Expression of Interest form.
Please get in touch if you want to discuss the accessibility of resources we offer to support you in delivering our qualifications.
\includegraphics{figure_13}
A conical shell, of semi-vertical angle $\alpha$, is fixed with its axis vertical and its vertex V upwards. A light inextensible string passes through a small smooth hole at V and a particle P of mass 4 kg hangs in equilibrium at one end of the string. The other end of the string is attached to a particle Q of mass 25 kg which moves in a horizontal circle at constant angular speed $2.8 \text{ rad s}^{-1}$ on the smooth outer surface of the shell at a vertical depth $h$ m below V (see diagram).
\begin{enumerate}[label=(\alph*)]
\item Show that $k_1 h \sin^2 \alpha + k_2 \cos^2 \alpha = k_3 \cos \alpha$, where $k_1$, $k_2$ and $k_3$ are integers to be determined. [7]
\item Determine the greatest value of $h$ for which Q remains in contact with the shell. [3]
\end{enumerate}
\hfill \mbox{\textit{OCR MEI Further Mechanics Major 2024 Q13 [10]}}