October 2021 Paper 1 Q13
13 In this question \(\mathbf{i}\) and \(\mathbf{j}\) are unit vectors in the \(x\)- and \(y\)-directions respectively.
The velocity of a particle at time \(t\) s is given by \((3t^2\mathbf{i} + 7\mathbf{j})\,\text{m}\,\text{s}^{-1}\). At time \(t = 0\) the position of the particle with respect to the origin is \((-\mathbf{i} + 2\mathbf{j})\) m.
Find the mass of the particle. [4]
| Scheme | Marks | AO |
|---|---|---|
| \(\mathbf{r} = \displaystyle\int(\mathbf{v})\,\mathrm{d}t = \int\left(3t^2\mathbf{i} + 7\mathbf{j}\right)\mathrm{d}t\) \(= t^3\mathbf{i} + 7t\mathbf{j} + \mathbf{c}\) | M1* | 3.4 |
| When \(t = 0,\ \mathbf{r} = -\mathbf{i} + 2\mathbf{j} = \mathbf{c}\) So \(\mathbf{r} = (t^3 - 1)\mathbf{i} + (7t + 2)\mathbf{j}\) | M1 dep* | 1.1b |
| When \(t = 2\), \(\mathbf{r} = (2^3 - 1)\mathbf{i} + (7 \times 2 + 2)\mathbf{j} = 7\mathbf{i} + 16\mathbf{j}\) | M1 dep* A1 | 3.1b 1.1b |
| distance \(= \sqrt{7^2 + 16^2} = \sqrt{305}\) | M1 | 3.1b |
| distance = 17.5 m | A1 | 3.2a |
| [6] |
Notes
M1*: Attempt to integrate both components; condone missing \(+\mathbf{c}\)
M1 dep*: Using initial conditions
M1 dep*: Using \(t = 2\) to find position vector or values for \(x\) and \(y\)
A1: Accept vector form or two clear components.
M1: Using Pythagoras
A1: FT their components
| Scheme | Marks | AO |
|---|---|---|
| using \(x = t^3 - 1,\ y = 7t + 2\) | M1 | 3.1a |
| Substitute \(t = \dfrac{y-2}{7}\) into equation for \(x\) | M1 dep | 1.1b |
| \(x = \left(\dfrac{y-2}{7}\right)^3 - 1\) AG | A1 | 1.1b |
| [3] |
Notes
M1: Extracting equations for \(x\) and \(y\) from their displacement vector
M1 dep: Attempt to eliminate \(t\)
A1: cao
Equivalent form \(y = 7(x+1)^{\frac{1}{3}} + 2\) for M1M1A0
| Scheme | Marks | AO |
|---|---|---|
| \(\mathbf{a} = \dfrac{\mathrm{d}\mathbf{v}}{\mathrm{d}t} = 6t\mathbf{i}\) | M1* | 3.1b |
| When \(t = 2,\ \mathbf{a} = 12\mathbf{i}\) | M1* | 3.4 |
| The force must be in that direction, so \(\mathbf{F} = 48\mathbf{i} = m\mathbf{a}\) | M1* | 3.1b |
| So \(m = 4\) kg | A1 dep* | 1.1b |
| [4] |
Notes
M1*: Must be vector acceleration
M1*: Evaluating when \(t = 2\)
\(a = 12\) is sufficient here
M1*: Newton’s second law in vector form, or in \(x\)-direction only
If their \(\mathbf{a}\) has two non-zero components, allow for dividing 48 by the magnitude of their \(\mathbf{a}\)
A1 dep*: cao