OCR MEI M3 2012 January — Question 1 18 marks

Exam BoardOCR MEI
ModuleM3 (Mechanics 3)
Year2012
SessionJanuary
Marks18
PaperDownload PDF ↗
Mark schemeDownload PDF ↗
TopicDimensional Analysis
TypeDerive dimensions from formula
DifficultyModerate -0.8 This is a straightforward dimensional analysis question requiring only systematic application of standard techniques: rearranging formulas to find dimensions, unit conversions using scale factors, checking dimensional consistency, and solving simultaneous equations from dimensional analysis. All parts are routine textbook exercises with no novel problem-solving required, making it easier than average despite being multi-part.
Spec6.01a Dimensions: M, L, T notation6.01c Dimensional analysis: error checking6.01d Unknown indices: using dimensions6.01e Formulate models: dimensional arguments

1 The surface tension of a liquid enables a metal needle to be at rest on the surface of the liquid. The greatest mass \(m\) of a needle of length \(a\) which can be supported in this way by a liquid of surface tension \(S\) is given by $$m = \frac { 2 S a } { g }$$ where \(g\) is the acceleration due to gravity.
  1. Show that the dimensions of surface tension are \(\mathrm { MT } ^ { - 2 }\). The surface tension of water is 0.073 when expressed in SI units (based on kilograms, metres and seconds).
  2. Find the surface tension of water when expressed in a system of units based on grams, centimetres and minutes. Liquid will rise up a capillary tube to a height \(h\) given by \(h = \frac { 2 S } { \rho g r }\), where \(\rho\) is the density of the liquid and \(r\) is the radius of the capillary tube. \(r\) is the radius of the capillary tube.
  3. Show that the equation \(h = \frac { 2 S } { \rho g r }\) is dimensionally consistent.
  4. Find the radius of a capillary tube in which water will rise to a height of 25 cm . (The density of water is 1000 in SI units.) When liquid is poured onto a horizontal surface, it forms puddles of depth \(d\). You are given that \(d = k S ^ { \alpha } \rho ^ { \beta } g ^ { \gamma }\) where \(k\) is a dimensionless constant.
  5. Use dimensional analysis to find \(\alpha , \beta\) and \(\gamma\). Water forms puddles of depth 0.44 cm . Mercury has surface tension 0.487 and density 13500 in SI units.
  6. Find the depth of puddles formed by mercury on a horizontal surface.

Question 1:
Part (i)
AnswerMarks Guidance
AnswerMarks Guidance
\([g] = LT^{-2}\)B1
\([S] = \left[\frac{mg}{2a}\right] = \frac{M(LT^{-2})}{L} = MT^{-2}\)M1, E1 Obtaining dimensions of \(S\)
Part (ii)
AnswerMarks Guidance
AnswerMarks Guidance
\(0.073 \times 1000 \times 60^2\)M1M1 For \(\times 1000\) and \(\times 60^2\); Give M1 for \(\frac{1}{1000} \times \frac{1}{60^2}\); 3 600 000 implies M2; \(2.8\times10^{-7}\) or \(2.0\times10^{-8}\) implies M1
\(= 262800\)A1
Part (iii)
AnswerMarks Guidance
AnswerMarks Guidance
\([\rho] = ML^{-3}\)B1
\([\text{RHS}] = \frac{MT^{-2}}{(ML^{-3})(LT^{-2})(L)} = L\)M1 Obtaining dimensions of RHS
\([\text{LHS}] = L\), so it is dimensionally consistentE1 Correctly shown
Part (iv)
AnswerMarks Guidance
AnswerMarks Guidance
\(r = \frac{2S}{\rho g h} = \frac{2\times0.073}{1000\times9.8\times0.25}\)M1 Correct explicit numerical expression for \(r\). May have 25 for \(h\)
\(= 5.96\times10^{-5}\) m (3 sf)A1
Part (v)
AnswerMarks Guidance
AnswerMarks Guidance
\(L = (MT^{-2})^\alpha (ML^{-3})^\beta (LT^{-2})^\gamma\)
\(\alpha+\beta=0,\quad -3\beta+\gamma=1,\quad -2\alpha-2\gamma=0\)M2 For 3 equations (give M1 for 2 equations); CAO
\(\alpha=\frac{1}{2},\quad \beta=-\frac{1}{2},\quad \gamma=-\frac{1}{2}\)A2 Give A1 (dep M2) for two correct; If \([\rho]\) and/or \([g]\) wrong, give A1 for at least two correct values FT
Part (vi)
AnswerMarks Guidance
AnswerMarks Guidance
\(d = kS^{\frac{1}{2}}\rho^{-\frac{1}{2}}g^{-\frac{1}{2}}\)
\(d=0.0044,\ S=0.073,\ \rho=1000,\ g=9.8 \Rightarrow k=1.612\)M1 Obtaining a value for \(k\); Or \(\left(\frac{0.487}{0.073}\right)^{\frac{1}{2}}\) or \(\left(\frac{13500}{1000}\right)^{-\frac{1}{2}}\)
\(d_M = 1.612\times0.487^{\frac{1}{2}}\times13500^{-\frac{1}{2}}\times9.8^{-\frac{1}{2}}\)M1 Obtaining expression for \(d_M\)
Depth for mercury is \(0.00309\) m (3 sf)A1 CAO or 0.31 cm; But A0 for 0.31 m
# Question 1:

## Part (i)
| Answer | Marks | Guidance |
|--------|-------|----------|
| $[g] = LT^{-2}$ | B1 | |
| $[S] = \left[\frac{mg}{2a}\right] = \frac{M(LT^{-2})}{L} = MT^{-2}$ | M1, E1 | Obtaining dimensions of $S$ |

## Part (ii)
| Answer | Marks | Guidance |
|--------|-------|----------|
| $0.073 \times 1000 \times 60^2$ | M1M1 | For $\times 1000$ and $\times 60^2$; Give M1 for $\frac{1}{1000} \times \frac{1}{60^2}$; 3 600 000 implies M2; $2.8\times10^{-7}$ or $2.0\times10^{-8}$ implies M1 |
| $= 262800$ | A1 | |

## Part (iii)
| Answer | Marks | Guidance |
|--------|-------|----------|
| $[\rho] = ML^{-3}$ | B1 | |
| $[\text{RHS}] = \frac{MT^{-2}}{(ML^{-3})(LT^{-2})(L)} = L$ | M1 | Obtaining dimensions of RHS |
| $[\text{LHS}] = L$, so it is dimensionally consistent | E1 | Correctly shown |

## Part (iv)
| Answer | Marks | Guidance |
|--------|-------|----------|
| $r = \frac{2S}{\rho g h} = \frac{2\times0.073}{1000\times9.8\times0.25}$ | M1 | Correct explicit numerical expression for $r$. May have 25 for $h$ |
| $= 5.96\times10^{-5}$ m (3 sf) | A1 | |

## Part (v)
| Answer | Marks | Guidance |
|--------|-------|----------|
| $L = (MT^{-2})^\alpha (ML^{-3})^\beta (LT^{-2})^\gamma$ | | |
| $\alpha+\beta=0,\quad -3\beta+\gamma=1,\quad -2\alpha-2\gamma=0$ | M2 | For 3 equations (give M1 for 2 equations); CAO |
| $\alpha=\frac{1}{2},\quad \beta=-\frac{1}{2},\quad \gamma=-\frac{1}{2}$ | A2 | Give A1 (dep M2) for two correct; If $[\rho]$ and/or $[g]$ wrong, give A1 for at least two correct values FT |

## Part (vi)
| Answer | Marks | Guidance |
|--------|-------|----------|
| $d = kS^{\frac{1}{2}}\rho^{-\frac{1}{2}}g^{-\frac{1}{2}}$ | | |
| $d=0.0044,\ S=0.073,\ \rho=1000,\ g=9.8 \Rightarrow k=1.612$ | M1 | Obtaining a value for $k$; Or $\left(\frac{0.487}{0.073}\right)^{\frac{1}{2}}$ or $\left(\frac{13500}{1000}\right)^{-\frac{1}{2}}$ |
| $d_M = 1.612\times0.487^{\frac{1}{2}}\times13500^{-\frac{1}{2}}\times9.8^{-\frac{1}{2}}$ | M1 | Obtaining expression for $d_M$ |
| Depth for mercury is $0.00309$ m (3 sf) | A1 | CAO or 0.31 cm; But A0 for 0.31 m |

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1 The surface tension of a liquid enables a metal needle to be at rest on the surface of the liquid. The greatest mass $m$ of a needle of length $a$ which can be supported in this way by a liquid of surface tension $S$ is given by

$$m = \frac { 2 S a } { g }$$

where $g$ is the acceleration due to gravity.\\
(i) Show that the dimensions of surface tension are $\mathrm { MT } ^ { - 2 }$.

The surface tension of water is 0.073 when expressed in SI units (based on kilograms, metres and seconds).\\
(ii) Find the surface tension of water when expressed in a system of units based on grams, centimetres and minutes.

Liquid will rise up a capillary tube to a height $h$ given by $h = \frac { 2 S } { \rho g r }$, where $\rho$ is the density of the liquid and\\
$r$ is the radius of the capillary tube. $r$ is the radius of the capillary tube.\\
(iii) Show that the equation $h = \frac { 2 S } { \rho g r }$ is dimensionally consistent.\\
(iv) Find the radius of a capillary tube in which water will rise to a height of 25 cm . (The density of water is 1000 in SI units.)

When liquid is poured onto a horizontal surface, it forms puddles of depth $d$. You are given that $d = k S ^ { \alpha } \rho ^ { \beta } g ^ { \gamma }$ where $k$ is a dimensionless constant.\\
(v) Use dimensional analysis to find $\alpha , \beta$ and $\gamma$.

Water forms puddles of depth 0.44 cm . Mercury has surface tension 0.487 and density 13500 in SI units.\\
(vi) Find the depth of puddles formed by mercury on a horizontal surface.

\hfill \mbox{\textit{OCR MEI M3 2012 Q1 [18]}}