OCR M4 2015 June — Question 5 15 marks

Exam BoardOCR
ModuleM4 (Mechanics 4)
Year2015
SessionJune
Marks15
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicSecond order differential equations
TypeFind turning points or extrema
DifficultyChallenging +1.8 This is a multi-part mechanics question requiring derivation of potential energy, finding equilibrium conditions by differentiation, analyzing parameter ranges for multiple equilibria, and stability analysis via second derivatives. It demands strong understanding of energy methods, trigonometric manipulation, and conceptual insight into stability—significantly harder than routine mechanics problems but standard for M4 level.
Spec3.04b Equilibrium: zero resultant moment and force6.02e Calculate KE and PE: using formulae6.05a Angular velocity: definitions

  1. Taking \(H\) as the reference level for gravitational potential energy, show that the total potential energy \(V\) of the system is given by $$V = m g \left( 2 \lambda r \cos \theta - 2 r \cos ^ { 2 } \theta - \lambda a \right)$$
  2. Find the set of possible values of \(\lambda\) so that there is more than one position of equilibrium.
  3. For the case \(\lambda = \frac { 3 } { 2 }\), determine whether each equilibrium position is stable or unstable.

Question 5:
Part (i):
AnswerMarks Guidance
AnswerMarks Guidance
\(HB = 2r\cos\theta\) and \(HP = a - 2r\cos\theta\)B1 B1
\(V = -\lambda mg(HP) - mg(HB)\cos\theta\)M1 Attempt at \(V\) with their \(HP\) and \(HB\)
\(V = -\lambda mg(a - 2r\cos\theta) - 2mgr\cos^2\theta\)A1 One term correct
\(V = mg(2\lambda r\cos\theta - 2r\cos^2\theta - \lambda a)\)A1 [5] AG www correctly obtained. If M0 then SC B1 for one term correct
Part (ii):
AnswerMarks Guidance
AnswerMarks Guidance
\(\dfrac{dV}{d\theta} = -2\lambda mgr\sin\theta + 4mgr\cos\theta\sin\theta = 0\)M1 Attempt at differentiation
\(2mgr\sin\theta(2\cos\theta - \lambda) = 0\)A1 Correct derivative and equal to zero
\(\frac{1}{2} \leq \cos\theta < 1\)M1 Comparing their \(\cos\theta < 1\) or \(\cos\theta \geq \frac{1}{2}\) - condone \(\cos\theta \leq 1\)
\(\Rightarrow 1 \leq \lambda < 2\)A1 [4]
Part (iii):
AnswerMarks Guidance
AnswerMarks Guidance
\(\dfrac{d^2V}{d\theta^2} = -2\left(\frac{3}{2}\right)mgr\cos\theta + 4mgr\cos2\theta\)*M1 A1 M1 Attempt to differentiate \(V'\) (or first derivative test) – allow in terms of \(\lambda\)
M1 dep*M1 sub. their first angle into \(V''\) (maybe implied by later working)
\(\sin\theta = 0 \Rightarrow V'' = mgr > 0\ \therefore\) stableA1 A1 correct (unsimplified) value of \(V''\) and \(> 0\)
M1 dep*M1 sub. their second angle into \(V''\) (maybe implied by later working)
\(\cos\theta = \frac{3}{4} \Rightarrow V'' = -\frac{7}{4}mgr < 0\ \therefore\) unstableA1 [6] A1 correct (unsimplified) value of \(V''\) and \(< 0\). If both values of \(V''\) correct and correct conclusion then award B1 if no consideration of sign seen
# Question 5:

## Part (i):
| Answer | Marks | Guidance |
|--------|-------|----------|
| $HB = 2r\cos\theta$ and $HP = a - 2r\cos\theta$ | B1 B1 | |
| $V = -\lambda mg(HP) - mg(HB)\cos\theta$ | M1 | Attempt at $V$ with their $HP$ and $HB$ |
| $V = -\lambda mg(a - 2r\cos\theta) - 2mgr\cos^2\theta$ | A1 | One term correct |
| $V = mg(2\lambda r\cos\theta - 2r\cos^2\theta - \lambda a)$ | A1 **[5]** | **AG www** correctly obtained. If M0 then SC B1 for one term correct |

## Part (ii):
| Answer | Marks | Guidance |
|--------|-------|----------|
| $\dfrac{dV}{d\theta} = -2\lambda mgr\sin\theta + 4mgr\cos\theta\sin\theta = 0$ | M1 | Attempt at differentiation |
| $2mgr\sin\theta(2\cos\theta - \lambda) = 0$ | A1 | Correct derivative and equal to zero |
| $\frac{1}{2} \leq \cos\theta < 1$ | M1 | Comparing their $\cos\theta < 1$ or $\cos\theta \geq \frac{1}{2}$ - condone $\cos\theta \leq 1$ |
| $\Rightarrow 1 \leq \lambda < 2$ | A1 **[4]** | |

## Part (iii):
| Answer | Marks | Guidance |
|--------|-------|----------|
| $\dfrac{d^2V}{d\theta^2} = -2\left(\frac{3}{2}\right)mgr\cos\theta + 4mgr\cos2\theta$ | *M1 A1 | M1 Attempt to differentiate $V'$ (or first derivative test) – allow in terms of $\lambda$ |
| | M1 dep* | M1 sub. their first angle into $V''$ (maybe implied by later working) |
| $\sin\theta = 0 \Rightarrow V'' = mgr > 0\ \therefore$ stable | A1 | A1 correct (unsimplified) value of $V''$ and $> 0$ |
| | M1 dep* | M1 sub. their second angle into $V''$ (maybe implied by later working) |
| $\cos\theta = \frac{3}{4} \Rightarrow V'' = -\frac{7}{4}mgr < 0\ \therefore$ unstable | A1 **[6]** | A1 correct (unsimplified) value of $V''$ and $< 0$. If both values of $V''$ correct and correct conclusion then award B1 if no consideration of sign seen |

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(i) Taking $H$ as the reference level for gravitational potential energy, show that the total potential energy $V$ of the system is given by

$$V = m g \left( 2 \lambda r \cos \theta - 2 r \cos ^ { 2 } \theta - \lambda a \right)$$

(ii) Find the set of possible values of $\lambda$ so that there is more than one position of equilibrium.\\
(iii) For the case $\lambda = \frac { 3 } { 2 }$, determine whether each equilibrium position is stable or unstable.

\hfill \mbox{\textit{OCR M4 2015 Q5 [15]}}