| Exam Board | Edexcel |
|---|---|
| Module | M3 (Mechanics 3) |
| Year | 2020 |
| Session | June |
| Marks | 10 |
| Paper | Download PDF ↗ |
| Mark scheme | Download PDF ↗ |
| Topic | Centre of Mass 2 |
| Type | Lamina with particle attached |
| Difficulty | Challenging +1.2 Part (a) is a standard M3 centre of mass derivation using disc integration with a given formula, requiring careful setup but routine execution. Part (b) involves equilibrium of a composite body with moments about the contact point, requiring geometric reasoning with the given angle. This is a typical M3 question combining standard techniques, slightly above average due to the 3D geometry and multi-part nature. |
| Spec | 6.04d Integration: for centre of mass of laminas/solids6.04e Rigid body equilibrium: coplanar forces |
| VIXV SIHIANI III IM IONOO | VIAV SIHI NI JYHAM ION OO | VI4V SIHI NI JLIYM ION OO |
| Answer | Marks | Guidance |
|---|---|---|
| Working/Answer | Mark | Guidance |
| \(M\bar{y} = (\rho)\pi\int_0^a y(a^2 - y^2)\,dy\) | M1 A1 | — |
| \(M\bar{y} = (\rho)\pi\left[\frac{a^2y^2}{2} - \frac{y^4}{4}\right]_0^a\) | A1 | — |
| \(\left(M\bar{y} = (\rho)\pi\frac{a^4}{4}\right)\) | — | — |
| \(\bar{y} = \frac{(\pi\rho)\frac{a^4}{4}}{(\pi\rho)\frac{2a^3}{3}} = \frac{3a}{8}\) | M1A1* | S.C. Clear use of \(r=1\) with \(a\) substituted at end can score max M1A0M1A0 |
| Answer | Marks | Guidance |
|---|---|---|
| Working/Answer | Mark | Guidance |
| \((k+1)m\bar{x} = kma \left(\Rightarrow \bar{x} = \frac{ka}{k+1}\right)\) | M1A1 | — |
| \((k+1)m\bar{y} = m\times\frac{3}{8}a \left(\Rightarrow \bar{y} = \frac{3a}{8(k+1)}\right)\) | A1 | — |
| \(\tan\alpha = \frac{\bar{x}}{\bar{y}}\) | M1 | — |
| \(k = \frac{3\sqrt{3}}{8}\) | A1 | — |
| Answer | Marks | Guidance |
|---|---|---|
| Working/Answer | Mark | Guidance |
| Moments about \(O\): \(m\times\frac{3a}{8}\sin\alpha = kma\times\cos\alpha\) | M1A2 | — |
| \(k = \frac{3\sqrt{3}}{8}\) | M1A1 | — |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| \((\pi)\int_0^r x^2 y \, dy\) | M1 | With or without \(\pi\). Must be dimensionally correct with integrand of form \(y(a^2 - y^2)\). Limits not needed. |
| \(\int_0^a y(a^2 - y^2) \, dx\) | A1 | Correct integral. Limits not needed. |
| Correct integration | A1 | Limits not needed. |
| \(\bar{y} = \dfrac{\int_0^a \pi x^2 y \, dy}{\frac{2}{3}\pi a^3}\) | M1 | \(\pi\) in numerator and denominator or in neither. |
| Correct given result with no errors seen | A1 | Cso |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| Dimensionally correct moments equation for \(\bar{x}\) or \(\bar{y}\) | M1 | First 3 marks can be awarded for equations only seen as part of a vector equation. |
| Correct equation in \(\bar{x}\) or \(\bar{y}\) | A1 | Give BOD on use of \(x\) and/or \(y\). |
| Correct equations for \(\bar{x}\) and \(\bar{y}\) | A1 | |
| Dividing to form equation in \(\tan\alpha\) and solve for \(k\) | M1 | Trig must be right. |
| \(k = \dfrac{3\sqrt{3}}{8}\) | A1 | Any correct exact form. |
| Answer | Marks | Guidance |
|---|---|---|
| Answer/Working | Mark | Guidance |
| Dimensionally correct moments equation about \(O\) | M1 | |
| Moments equation with at most one error | A1 | |
| Fully correct equation | A1 | |
| Solve for \(k\) | M1 | |
| c.a.o. | A1 |
## Question 4(a):
| Working/Answer | Mark | Guidance |
|---|---|---|
| $M\bar{y} = (\rho)\pi\int_0^a y(a^2 - y^2)\,dy$ | M1 A1 | — |
| $M\bar{y} = (\rho)\pi\left[\frac{a^2y^2}{2} - \frac{y^4}{4}\right]_0^a$ | A1 | — |
| $\left(M\bar{y} = (\rho)\pi\frac{a^4}{4}\right)$ | — | — |
| $\bar{y} = \frac{(\pi\rho)\frac{a^4}{4}}{(\pi\rho)\frac{2a^3}{3}} = \frac{3a}{8}$ | M1A1* | S.C. Clear use of $r=1$ with $a$ substituted at end can score max M1A0M1A0 |
**(5)**
## Question 4(b):
| Working/Answer | Mark | Guidance |
|---|---|---|
| $(k+1)m\bar{x} = kma \left(\Rightarrow \bar{x} = \frac{ka}{k+1}\right)$ | M1A1 | — |
| $(k+1)m\bar{y} = m\times\frac{3}{8}a \left(\Rightarrow \bar{y} = \frac{3a}{8(k+1)}\right)$ | A1 | — |
| $\tan\alpha = \frac{\bar{x}}{\bar{y}}$ | M1 | — |
| $k = \frac{3\sqrt{3}}{8}$ | A1 | — |
**(5) [10]**
**Alt b:**
| Working/Answer | Mark | Guidance |
|---|---|---|
| Moments about $O$: $m\times\frac{3a}{8}\sin\alpha = kma\times\cos\alpha$ | M1A2 | — |
| $k = \frac{3\sqrt{3}}{8}$ | M1A1 | — |
# Question (Centre of Mass - Part a):
| Answer/Working | Mark | Guidance |
|---|---|---|
| $(\pi)\int_0^r x^2 y \, dy$ | M1 | With or without $\pi$. Must be dimensionally correct with integrand of form $y(a^2 - y^2)$. Limits not needed. |
| $\int_0^a y(a^2 - y^2) \, dx$ | A1 | Correct integral. Limits not needed. |
| Correct integration | A1 | Limits not needed. |
| $\bar{y} = \dfrac{\int_0^a \pi x^2 y \, dy}{\frac{2}{3}\pi a^3}$ | M1 | $\pi$ in numerator and denominator or in neither. |
| Correct given result with no errors seen | A1 | **Cso** |
---
# Question (Centre of Mass - Part b):
| Answer/Working | Mark | Guidance |
|---|---|---|
| Dimensionally correct moments equation for $\bar{x}$ or $\bar{y}$ | M1 | First 3 marks can be awarded for equations only seen as part of a vector equation. |
| Correct equation in $\bar{x}$ or $\bar{y}$ | A1 | Give BOD on use of $x$ and/or $y$. |
| Correct equations for $\bar{x}$ and $\bar{y}$ | A1 | |
| Dividing to form equation in $\tan\alpha$ and solve for $k$ | M1 | Trig must be right. |
| $k = \dfrac{3\sqrt{3}}{8}$ | A1 | Any correct exact form. |
**ALT b) - Taking moments about O:**
| Answer/Working | Mark | Guidance |
|---|---|---|
| Dimensionally correct moments equation about $O$ | M1 | |
| Moments equation with at most one error | A1 | |
| Fully correct equation | A1 | |
| Solve for $k$ | M1 | |
| c.a.o. | A1 | |
---
4. (a) Use algebraic integration to show that the centre of mass of a uniform solid hemisphere of radius $a$ is a distance $\frac { 3 } { 8 } a$ from the centre of its plane face.\\[0pt]
[You may assume that the volume of a sphere of radius $r$ is $\frac { 4 } { 3 } \pi r ^ { 3 }$ ]
\begin{figure}[h]
\begin{center}
\includegraphics[alt={},max width=\textwidth]{ace84823-db30-463e-b24b-f0cd7df73746-08_444_764_539_591}
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\caption{Figure 4}
\end{center}
\end{figure}
A uniform solid hemisphere has mass $m$ and radius $a$. A particle of mass $k m$ is attached to a point $A$ on the circumference of the plane face of the hemisphere to form the loaded solid $S$. The centre of the plane face of the hemisphere is the point $O$, as shown in Figure 4.
The loaded solid $S$ is placed on a horizontal plane. The curved surface of $S$ is in contact with the plane and $S$ rests in equilibrium with $O A$ making an angle $\alpha$ with the horizontal, where $\tan \alpha = \sqrt { 3 }$\\
(b) Find the exact value of $k$.\\
\includegraphics[max width=\textwidth, alt={}, center]{ace84823-db30-463e-b24b-f0cd7df73746-09_2255_50_314_34}\\
\begin{center}
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VIXV SIHIANI III IM IONOO & VIAV SIHI NI JYHAM ION OO & VI4V SIHI NI JLIYM ION OO \\
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\end{center}
\hfill \mbox{\textit{Edexcel M3 2020 Q4 [10]}}