OCR M3 2007 June — Question 6 13 marks

Exam BoardOCR
ModuleM3 (Mechanics 3)
Year2007
SessionJune
Marks13
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicHooke's law and elastic energy
TypeBungee jumping problems
DifficultyChallenging +1.8 This is a multi-part bungee jumping problem requiring energy conservation across multiple phases, equilibrium analysis with elastic strings, and verification of specific outcomes. The problem demands careful bookkeeping of gravitational PE, elastic PE, and KE through several stages, plus the insight to apply energy methods after Q is released. The 'prove that P just reaches O' requires working backwards from final conditions, which is more sophisticated than routine energy problems.
Spec6.02i Conservation of energy: mechanical energy principle6.05d Variable speed circles: energy methods

  1. Show that, when \(P\) is in equilibrium, \(O P = 7.25 \mathrm {~m}\).
  2. Verify that \(P\) and \(Q\) together just reach the safety net.
  3. At the lowest point of their motion \(P\) releases \(Q\). Prove that \(P\) subsequently just reaches \(O\).
  4. State two additional modelling assumptions made when answering this question.

Question 6:
Part (i)
AnswerMarks Guidance
Answer/WorkingMark Guidance
\([T = 2058x/5.25]\)M1 For using \(T = \lambda x/L\)
\(2058x/5.25 = 80 \times 9.8 \quad (x = 2)\)A1
\(OP = 7.25\text{m}\)A1 [3 marks total] AG From \(5.25 + 2\)
Part (ii)
AnswerMarks Guidance
Answer/WorkingMark Guidance
Initial \(PE = (80 + 80)g(5) \quad (= 7840)\) or \((80+80)gX\) used in energy equationB1
Initial \(KE = \frac{1}{2}(80+80)3.5^2 \quad (= 980)\)B1
[Initial \(EE = 2058x^2/(2\times 5.25) \quad (= 784)\), Final \(EE = 2058 \times 7^2/(2\times 5.25) \quad (= 9604)\), or \(2058(X+2)^2/(2\times 5.25)\)]M1 For using \(EE = \lambda x^2/2L\)
[Initial energy \(= 7840 + 980 + 784\), final energy \(= 9604\)] or \(1568X + 980 + 784 = 196(X^2 + 4X + 4) \rightarrow 196X^2 - 784X - 980 = 0\)M1 For attempting to verify compatibility with the principle of conservation of energy, or using the principle and solving for X
Initial energy \(=\) final energy or \(X = 5 \rightarrow\) P&Q just reach the netA1 [5 marks total] AG
Part (iii)
AnswerMarks Guidance
Answer/WorkingMark Guidance
\([PE\text{ gain} = 80g(7.25 + 5)]\)M1 For finding PE gain from net level to O
\(PE\text{ gain} = 9604\)A1
\(PE\text{ gain} = EE\text{ at net level} \rightarrow\) P just reaches OA1 [3 marks total] AG
Part (iv)
AnswerMarks Guidance
Answer/WorkingMark Guidance
For any one of 'light rope', 'no air resistance', 'no energy lost in rope'B1
For any other of the aboveB1 [2 marks total]
First Alternative Method for Part (ii)
AnswerMarks Guidance
Answer/WorkingMark Guidance
\([160g - 2058x/5.25 = 160v\,dv/dx]\)M1 For using Newton's second law with \(a = v\,dv/dx\), separating the variables and attempting to integrate
\(v^2/2 = gx - 1.225x^2 \quad (+C)\)A1 Any correct form
M1For using \(v(2) = 3.5\)
\(C = -8.575\)A1
\([v(7)^2]/2 = 68.6 - 60.025 - 8.575 = 0 \rightarrow\) P&Q just reach the netA1 [5 marks total] AG
Second Alternative Method for Part (ii)
AnswerMarks Guidance
Answer/WorkingMark Guidance
\(\ddot{x} = g - 2.45x \quad (= -2.45(x-4))\)B1
M1For using \(n^2 = 2.45\) and \(v^2 = n^2(A^2 - (x-4)^2)\)
\(3.5^2 = 2.45(A^2 - (-2)^2) \quad (A = 3)\)A1
\([(4-2)+3]\)M1 For using 'distance travelled downwards by P and Q \(=\) distance to new equilibrium position \(+ A\)'
distance travelled downwards by P and Q \(= 5 \rightarrow\) P&Q just reach the netA1 [5 marks total] AG
# Question 6:

## Part (i)
| Answer/Working | Mark | Guidance |
|---|---|---|
| $[T = 2058x/5.25]$ | M1 | For using $T = \lambda x/L$ |
| $2058x/5.25 = 80 \times 9.8 \quad (x = 2)$ | A1 | |
| $OP = 7.25\text{m}$ | A1 | [3 marks total] AG From $5.25 + 2$ |

## Part (ii)
| Answer/Working | Mark | Guidance |
|---|---|---|
| Initial $PE = (80 + 80)g(5) \quad (= 7840)$ or $(80+80)gX$ used in energy equation | B1 | |
| Initial $KE = \frac{1}{2}(80+80)3.5^2 \quad (= 980)$ | B1 | |
| [Initial $EE = 2058x^2/(2\times 5.25) \quad (= 784)$, Final $EE = 2058 \times 7^2/(2\times 5.25) \quad (= 9604)$, or $2058(X+2)^2/(2\times 5.25)$] | M1 | For using $EE = \lambda x^2/2L$ |
| [Initial energy $= 7840 + 980 + 784$, final energy $= 9604$] or $1568X + 980 + 784 = 196(X^2 + 4X + 4) \rightarrow 196X^2 - 784X - 980 = 0$ | M1 | For attempting to verify compatibility with the principle of conservation of energy, or using the principle and solving for X |
| Initial energy $=$ final energy or $X = 5 \rightarrow$ P&Q just reach the net | A1 | [5 marks total] AG |

## Part (iii)
| Answer/Working | Mark | Guidance |
|---|---|---|
| $[PE\text{ gain} = 80g(7.25 + 5)]$ | M1 | For finding PE gain from net level to O |
| $PE\text{ gain} = 9604$ | A1 | |
| $PE\text{ gain} = EE\text{ at net level} \rightarrow$ P just reaches O | A1 | [3 marks total] AG |

## Part (iv)
| Answer/Working | Mark | Guidance |
|---|---|---|
| For any one of 'light rope', 'no air resistance', 'no energy lost in rope' | B1 | |
| For any other of the above | B1 | [2 marks total] |

## First Alternative Method for Part (ii)
| Answer/Working | Mark | Guidance |
|---|---|---|
| $[160g - 2058x/5.25 = 160v\,dv/dx]$ | M1 | For using Newton's second law with $a = v\,dv/dx$, separating the variables and attempting to integrate |
| $v^2/2 = gx - 1.225x^2 \quad (+C)$ | A1 | Any correct form |
| | M1 | For using $v(2) = 3.5$ |
| $C = -8.575$ | A1 | |
| $[v(7)^2]/2 = 68.6 - 60.025 - 8.575 = 0 \rightarrow$ P&Q just reach the net | A1 | [5 marks total] AG |

## Second Alternative Method for Part (ii)
| Answer/Working | Mark | Guidance |
|---|---|---|
| $\ddot{x} = g - 2.45x \quad (= -2.45(x-4))$ | B1 | |
| | M1 | For using $n^2 = 2.45$ and $v^2 = n^2(A^2 - (x-4)^2)$ |
| $3.5^2 = 2.45(A^2 - (-2)^2) \quad (A = 3)$ | A1 | |
| $[(4-2)+3]$ | M1 | For using 'distance travelled downwards by P and Q $=$ distance to new equilibrium position $+ A$' |
| distance travelled downwards by P and Q $= 5 \rightarrow$ P&Q just reach the net | A1 | [5 marks total] AG |

---
(i) Show that, when $P$ is in equilibrium, $O P = 7.25 \mathrm {~m}$.\\
(ii) Verify that $P$ and $Q$ together just reach the safety net.\\
(iii) At the lowest point of their motion $P$ releases $Q$. Prove that $P$ subsequently just reaches $O$.\\
(iv) State two additional modelling assumptions made when answering this question.

\hfill \mbox{\textit{OCR M3 2007 Q6 [13]}}