OCR MEI M3 2006 June — Question 3 18 marks

Exam BoardOCR MEI
ModuleM3 (Mechanics 3)
Year2006
SessionJune
Marks18
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicSimple Harmonic Motion
TypeVertical SHM with two strings
DifficultyChallenging +1.2 This is a standard Further Maths Mechanics 3 vertical SHM question with two elastic strings. While it requires multiple techniques (equilibrium verification, tension formulas, SHM equation derivation, and energy/kinematics), each part follows predictable patterns taught in M3. The multi-part structure and need to track two strings simultaneously elevates it slightly above average difficulty, but it remains a textbook-style question without requiring novel insight.
Spec4.10f Simple harmonic motion: x'' = -omega^2 x6.02g Hooke's law: T = k*x or T = lambda*x/l6.02h Elastic PE: 1/2 k x^26.02i Conservation of energy: mechanical energy principle

3 A fixed point A is 12 m vertically above a fixed point B. A light elastic string, with natural length 3 m and modulus of elasticity 1323 N , has one end attached to A and the other end attached to a particle P of mass 15 kg . Another light elastic string, with natural length 4.5 m and modulus of elasticity 1323 N , has one end attached to B and the other end attached to P .
  1. Verify that, in the equilibrium position, \(\mathrm { AP } = 5 \mathrm {~m}\). The particle P now moves vertically, with both strings AP and BP remaining taut throughout the motion. The displacement of P above the equilibrium position is denoted by \(x \mathrm {~m}\) (see Fig. 3). \begin{figure}[h]
    \includegraphics[alt={},max width=\textwidth]{5bb02383-91c0-4454-aaea-0bd6af6ba325-4_405_360_751_849} \captionsetup{labelformat=empty} \caption{Fig. 3}
    \end{figure}
  2. Show that the tension in the string AP is \(441 ( 2 - x ) \mathrm { N }\) and find the tension in the string BP .
  3. Show that the motion of P is simple harmonic, and state the period. The minimum length of AP during the motion is 3.5 m .
  4. Find the maximum length of AP .
  5. Find the speed of P when \(\mathrm { AP } = 4.1 \mathrm {~m}\).
  6. Find the time taken for AP to increase from 3.5 m to 4.5 m .

Question 3:
Part (i) - Verify AP = 5 m
AnswerMarks Guidance
AnswerMark Guidance
Tension in AP: \(T_{AP} = \dfrac{1323(AP - 3)}{3}\)M1 Using \(T = \frac{\lambda e}{l_0}\)
Tension in BP: \(T_{BP} = \dfrac{1323(BP - 4.5)}{4.5}\), where \(BP = 12 - AP\)A1
Equilibrium: \(T_{AP} = T_{BP} + 15g\)M1
\(\dfrac{1323(AP-3)}{3} = \dfrac{1323(12-AP-4.5)}{4.5} + 147\)A1
Solving gives \(AP = 5\) m ✓A1
Part (ii) - Tensions
AnswerMarks Guidance
AnswerMark Guidance
\(AP = 5 + x\), extension in AP \(= (2+x)\) mM1
\(T_{AP} = \dfrac{1323(2+x)}{3} = 441(2+x)\) NA1
\(BP = 7 - x\), extension in BP \(= (7-x-4.5) = (2.5-x)\) mM1
\(T_{BP} = \dfrac{1323(2.5-x)}{4.5} = 294(2.5-x)\) NA1
Part (iii) - Simple harmonic motion and period
AnswerMarks Guidance
AnswerMark Guidance
Net upward force \(= T_{AP} - T_{BP} - 15g\)M1
\(= 441(2+x) - 294(2.5-x) - 147\)A1
\(= 882 + 441x - 735 + 294x - 147 = 735x\)A1
\(15\ddot{x} = -735x \Rightarrow \ddot{x} = -49x\)M1 SHM condition
\(\omega^2 = 49\), \(T = \dfrac{2\pi}{7} \approx 0.898\) sA1
Part (iv) - Maximum length of AP
AnswerMarks Guidance
AnswerMark Guidance
Min AP \(= 3.5\) m \(\Rightarrow x = -1.5\) m (amplitude \(= 1.5\) m)M1
Max AP \(= 5 + 1.5 = 6.5\) mA1
Part (v) - Speed when AP = 4.1 m
AnswerMarks Guidance
AnswerMark Guidance
\(x = 4.1 - 5 = -0.9\) mB1
\(v^2 = \omega^2(a^2 - x^2) = 49(1.5^2 - 0.9^2)\)M1
\(v^2 = 49(2.25 - 0.81) = 49 \times 1.44 = 70.56\)A1
\(v = 8.4\) ms\(^{-1}\)A1
Part (vi) - Time for AP to increase from 3.5 m to 4.5 m
AnswerMarks Guidance
AnswerMark Guidance
\(x = -1.5\) when \(AP = 3.5\): \(x = -1.5\cos(7t)\)M1 Starting from minimum
When \(AP = 4.5\): \(x = -0.5\), so \(-0.5 = -1.5\cos(7t)\)M1
\(\cos(7t) = \dfrac{1}{3}\)A1
\(t = \dfrac{1}{7}\arccos\!\left(\dfrac{1}{3}\right) = \dfrac{1.2310}{7} \approx 0.176\) sA1
# Question 3:

## Part (i) - Verify AP = 5 m

| Answer | Mark | Guidance |
|--------|------|----------|
| Tension in AP: $T_{AP} = \dfrac{1323(AP - 3)}{3}$ | M1 | Using $T = \frac{\lambda e}{l_0}$ |
| Tension in BP: $T_{BP} = \dfrac{1323(BP - 4.5)}{4.5}$, where $BP = 12 - AP$ | A1 | |
| Equilibrium: $T_{AP} = T_{BP} + 15g$ | M1 | |
| $\dfrac{1323(AP-3)}{3} = \dfrac{1323(12-AP-4.5)}{4.5} + 147$ | A1 | |
| Solving gives $AP = 5$ m ✓ | A1 | |

## Part (ii) - Tensions

| Answer | Mark | Guidance |
|--------|------|----------|
| $AP = 5 + x$, extension in AP $= (2+x)$ m | M1 | |
| $T_{AP} = \dfrac{1323(2+x)}{3} = 441(2+x)$ N | A1 | |
| $BP = 7 - x$, extension in BP $= (7-x-4.5) = (2.5-x)$ m | M1 | |
| $T_{BP} = \dfrac{1323(2.5-x)}{4.5} = 294(2.5-x)$ N | A1 | |

## Part (iii) - Simple harmonic motion and period

| Answer | Mark | Guidance |
|--------|------|----------|
| Net upward force $= T_{AP} - T_{BP} - 15g$ | M1 | |
| $= 441(2+x) - 294(2.5-x) - 147$ | A1 | |
| $= 882 + 441x - 735 + 294x - 147 = 735x$ | A1 | |
| $15\ddot{x} = -735x \Rightarrow \ddot{x} = -49x$ | M1 | SHM condition |
| $\omega^2 = 49$, $T = \dfrac{2\pi}{7} \approx 0.898$ s | A1 | |

## Part (iv) - Maximum length of AP

| Answer | Mark | Guidance |
|--------|------|----------|
| Min AP $= 3.5$ m $\Rightarrow x = -1.5$ m (amplitude $= 1.5$ m) | M1 | |
| Max AP $= 5 + 1.5 = 6.5$ m | A1 | |

## Part (v) - Speed when AP = 4.1 m

| Answer | Mark | Guidance |
|--------|------|----------|
| $x = 4.1 - 5 = -0.9$ m | B1 | |
| $v^2 = \omega^2(a^2 - x^2) = 49(1.5^2 - 0.9^2)$ | M1 | |
| $v^2 = 49(2.25 - 0.81) = 49 \times 1.44 = 70.56$ | A1 | |
| $v = 8.4$ ms$^{-1}$ | A1 | |

## Part (vi) - Time for AP to increase from 3.5 m to 4.5 m

| Answer | Mark | Guidance |
|--------|------|----------|
| $x = -1.5$ when $AP = 3.5$: $x = -1.5\cos(7t)$ | M1 | Starting from minimum |
| When $AP = 4.5$: $x = -0.5$, so $-0.5 = -1.5\cos(7t)$ | M1 | |
| $\cos(7t) = \dfrac{1}{3}$ | A1 | |
| $t = \dfrac{1}{7}\arccos\!\left(\dfrac{1}{3}\right) = \dfrac{1.2310}{7} \approx 0.176$ s | A1 | |

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3 A fixed point A is 12 m vertically above a fixed point B. A light elastic string, with natural length 3 m and modulus of elasticity 1323 N , has one end attached to A and the other end attached to a particle P of mass 15 kg . Another light elastic string, with natural length 4.5 m and modulus of elasticity 1323 N , has one end attached to B and the other end attached to P .\\
(i) Verify that, in the equilibrium position, $\mathrm { AP } = 5 \mathrm {~m}$.

The particle P now moves vertically, with both strings AP and BP remaining taut throughout the motion. The displacement of P above the equilibrium position is denoted by $x \mathrm {~m}$ (see Fig. 3).

\begin{figure}[h]
\begin{center}
  \includegraphics[alt={},max width=\textwidth]{5bb02383-91c0-4454-aaea-0bd6af6ba325-4_405_360_751_849}
\captionsetup{labelformat=empty}
\caption{Fig. 3}
\end{center}
\end{figure}

(ii) Show that the tension in the string AP is $441 ( 2 - x ) \mathrm { N }$ and find the tension in the string BP .\\
(iii) Show that the motion of P is simple harmonic, and state the period.

The minimum length of AP during the motion is 3.5 m .\\
(iv) Find the maximum length of AP .\\
(v) Find the speed of P when $\mathrm { AP } = 4.1 \mathrm {~m}$.\\
(vi) Find the time taken for AP to increase from 3.5 m to 4.5 m .

\hfill \mbox{\textit{OCR MEI M3 2006 Q3 [18]}}