3. A particle of mass 0.6 kg is moving with constant velocity ( \(c \mathbf { i } + 2 c \mathbf { j }\) ) \(\mathrm { ms } ^ { - 1 }\), where \(c\) is a positive constant. The particle receives an impulse of magnitude \(2 \sqrt { 10 } \mathrm {~N} \mathrm {~s}\). Immediately after receiving the impulse the particle has velocity ( \(2 c \mathbf { i } - c \mathbf { j }\) ) \(\mathrm { ms } ^ { - 1 }\).
Find the value of \(c\).
(6)
Show mark scheme
Show mark scheme source
Since this question is about the magnitude of the impulse, condone subtraction in the "wrong order" throughout.
Answer Marks
Guidance
\(m\mathbf{v} - m\mathbf{u} = 0.6(2c\mathbf{i} - c\mathbf{j} - c\mathbf{i} - 2c\mathbf{j})\) M1
Impulse = change in momentum. Marking the RHS only
\(= 0.6(c\mathbf{i} - 3c\mathbf{j})\) A1
Magnitude \(= 0.6\sqrt{c^2 + 9c^2}\) DM1
Correct use of Pythagoras' theorem on \(m\mathbf{v} - m\mathbf{u}\) or \(\mathbf{v} - \mathbf{u}\). Marking the RHS only. Dependent on the previous M1
\(= 0.6\sqrt{10c} = (-0.6\sqrt{10c^2})\) A1
Accept \(\sqrt{10}c\) for change in velocity
The next two marks are not available to a candidate who has equated a scalar to a vector.
\(2\sqrt{10} = 0.6\sqrt{10}c\) DM1
Equate & solve for \(c\). Dependent on the previous M1
\(c = \frac{10}{3}\) A1
Accept 3.3 or better
(6)
Question 3 alt
Answer Marks
Guidance
\(m\mathbf{v} - m\mathbf{u} = 0.6(2c\mathbf{i} - c\mathbf{j} - c\mathbf{i} - 2c\mathbf{j})\) M1
change in momentum
\(= 0.6(c\mathbf{i} - 3c\mathbf{j})\) A1
Square of magnitude DM1
\(= 0.36(10c^2)\) A1
The next two marks are not available to a candidate who has equated a scalar to a vector.
\(40 = 0.36(c^2 + 9c^2)\) DM1
Equate & solve for \(c\)
\(c = \frac{10}{3}\) A1
(6)
Question 3 alt (impulse momentum equation)
Answer Marks
Guidance
\(\begin{pmatrix} 2\sqrt{10} \cos \theta \\ 2\sqrt{10} \sin \theta \end{pmatrix} = 0.6 \begin{pmatrix} 2c - c \\ -c - 2c \end{pmatrix}\) M1
Impulse momentum equation
\(= 0.6c \begin{pmatrix} 1 \\ -3 \end{pmatrix}\) A1
Correct equation
\(2\sqrt{10} \cos \theta = 0.6c\) DM1
Compare coefficients and form equation for \(\theta\)
\(2\sqrt{10} \sin \theta = -3 \times 0.6c\)
\(\tan \theta = -3 \Rightarrow \cos \theta = (\pm) \frac{1}{\sqrt{10}}\) A1
\(\cos \theta\) or \(\sin \theta\) correct
\(2\sqrt{10} \cos \theta = 0.6c\) DM1
\(\Rightarrow c = \frac{10}{3}\) A1
Question 3 alt (impulse momentum triangle)
Answer Marks
Guidance
Impulse momentum triangle. Units used for the vectors must be dimensionally correct M1
Sides of magnitude \(\sqrt{5c}, \sqrt{5c}, \frac{10\sqrt{10}}{3}\) or \(\frac{3\sqrt{5c}}{5}, \frac{3\sqrt{5c}}{5}, 2\sqrt{10}\) A1
\(\mathbf{u} \cdot \mathbf{v} = \begin{pmatrix} c \\ 2c \end{pmatrix} \cdot \begin{pmatrix} 2c \\ -c \end{pmatrix}\) DM1
Use of scalar product
\(= 2c^2 - 2c^2 = 0 \therefore\) at \(90°\) A1
...to show velocities perpendicular. Use of Pythagoras' theorem in a right angled triangle
\((0.6 \times \sqrt{5c})^2 + (0.6 \times \sqrt{5c})^2 = (2\sqrt{10})^2\) DM1
\(\frac{18c^2}{5} = 40, c = \frac{10}{3}\) A1
(6)
Question 4a
Answer Marks
Guidance
Triangle sector
mass 4.5
\(4\pi\) (= 12.56..)
c of m from O \(\frac{2}{3}, \frac{3\sqrt{2}}{2}\) (= 1.41...)
\(\frac{16\sqrt{2}}{3\pi}\) (= 2.40....)
B1 Mass ratios
B1 Distances
Distances from \(AD\) are \(-\frac{1}{3} \times \frac{3\sqrt{2}}{2}\) and \(\frac{16\sqrt{2}}{3\pi} - \frac{3\sqrt{2}}{2}\) (= 0.280)
\(4\pi \times \frac{16\sqrt{2}}{3\pi} - 4.5\sqrt{2} = \left(\frac{101\sqrt{2}}{6}\right) = (4\pi - 4.5)d\) M1
Moments about an axis through O and parallel to DA. Terms must be dimensionally correct. Shapes combined correctly.
A1 Correct unsimplified equation
\(d = \frac{101\sqrt{2}}{6(4\pi - 4.5)} = 2.951.....\)
(distance from O)
Distance from \(DA = 2.951... - \frac{3\sqrt{2}}{2} = 0.830 \text{ (0.83) m}\) A1
Accept \(\frac{101\sqrt{2}}{6(4\pi - 4.5)} - \frac{3\sqrt{2}}{2}\)
(5)
Question 4a alt
Answer Marks
Guidance
Triangle sector
mass 4.5
\(4\pi (= 12.56..)\)
c of m from both axes \(OC, OB\) 1
\(\frac{16\sqrt{2}}{3\pi} \times \frac{1}{\sqrt{2}} = \frac{16}{3\pi}\)
\(4\pi \times \frac{16}{3\pi} - 4.5 \times 1 = (4\pi - 4.5)\bar{x}\) M1
Moments about an axis through O. Terms must be dimensionally correct. Condone sign error(s)
\((\bar{x} = \bar{y} = \frac{101}{6(4\pi - 4.5)})\) A1
Correct unsimplified equation
\(d = \frac{101\sqrt{2}}{6(4\pi - 4.5)}\)
Distance from O
Distance from \(DA = 2.951... - \frac{3\sqrt{2}}{2} = 0.830 \text{ (0.83) m}\) A1
(5)
Question 4b
Answer Marks
Guidance
\(\tan \theta = \frac{\text{their } 0.830}{2.12}\) or \(\tan \phi = \frac{2.12}{\text{their } 0.830}\) M1
Use of tan to find a relevant angle:
\(21.4°\) or \(68.6°\) A1
Angle between DC and downward vertical = \(135° -\) their \(\theta\) M1
Correct method for the required angle
\(= 114°\) A1
The Q asks for the angle to the nearest degree.
(4)
Question 4b alt
Answer Marks
Guidance
\(GD^2 = OD^2 + OG^2 - 2OD \cdot OG \cos 45\) M1
Complete method to find angle \(ODG\)
\((GD = 2.28)\)
\(\sin 45 = \frac{\sin \theta}{DG}\) and \(\frac{\sin \theta}{OG}\)
\(\Rightarrow \theta = 66.4°\) A1
Required angle = \(180° - 66.4° = 114°\) M1 A1
Correct method for the required angle. The Q asks for the angle to the nearest degree.
(4) [9]
Question 5a
Answer Marks
Guidance
M(A): \(d \cos \theta \times 5g = 4P\) M1
Terms must be dimensionally correct. Condone trig confusion
Resolving horizontally: \(P \sin \theta = F\) B1
Resolving vertically: \(P \cos \theta + R = 5g\) M1
Requires all 3 terms. Condone trig confusion and sign errors
A1 Correct equation
DM1 Substitute for \(P\) to find \(R\) or \(F\). Dependent on both previous M marks. One force correct. Accept equivalent forms e.g. \(R = \frac{20g - 5gd + 20g \tan^2 \theta}{4(1 + \tan^2 \theta)}\)
\(R = 5g - \frac{5gd \cos^2 \theta}{4}\) A1
One force correct
\(F = \frac{5gd \cos \theta \sin \theta}{4}\) A1
Both forces correct. Accept equivalent forms e.g. \(F = \frac{5gd \tan \theta}{4 \sec^2 \theta}\)
(8)
Question 5a alt
Answer Marks
Guidance
M(B): M1
Needs all three terms. Terms must be dimensionally correct. Condone trig confusion
\(5g \cos \theta \times (4 - d) + F \sin \theta \times 4 = R \cos \theta \times 4\)
Resolve parallel to the rod: M1
Requires all 3 terms. Condone trig confusion and sign errors
\(5g \sin \theta = R \sin \theta + F \cos \theta\) B1
At most one error
A1 Correct equation
\(\Rightarrow R = 5g - \frac{F \cos \theta}{\sin \theta}\)
\(5g \cos \theta \times (4 - d) + F \sin \theta \times 4 = 4 \cos \theta \left(5g - \frac{F \cos \theta}{\sin \theta}\right)\) DM1
Eliminate one variable to find \(F\) or \(R\). Dependent on both previous M marks
\(4F \left(\sin \theta + \frac{\cos^2 \theta}{\sin \theta}\right) = 20g \cos \theta - 20g \cos \theta + 5gd \cos \theta\)
\(= 20g \cos \theta - 20g \cos \theta + 5gd \cos \theta\)
\(F = \frac{5gd \cos \theta \sin \theta}{4}\) A1
One force correct
\(R = 5g - \frac{5gd \cos^2 \theta}{4}\) A1
Both forces correct
Question 5b
Answer Marks
Guidance
\(\mu = \frac{\frac{5gd \cos \theta \sin \theta}{4}}{5g - \frac{5gd \cos^2 \theta}{4}}\) M1
Use of \(F = \mu R\)
\(\frac{1}{2}\left(5g - \frac{5gd \cos^2 \theta}{4}\right) = \frac{5gd \cos \theta \sin \theta}{4}\) A1
\((4 - d \cos^2 \theta = 2d \cos \theta \sin \theta)\)
\(4 \times 169 - 120d + 144d\) M1
Use \(\tan \theta = \frac{5}{12}\) and solve for \(d\)
\(d = \frac{169}{66}\) A1
(= 2.6 m or better)
(4)
Question 5b alt
Answer Marks
Guidance
\(F = 5gd \times \frac{12}{13} \times \frac{5}{13} \times \frac{1}{4} = \left(\frac{75gd}{169}\right)\) M1
Use \(\tan \theta = \frac{5}{12}\)
\(R = 5g - \frac{5gd}{4} \times \frac{144}{169}\) A1
Both unsimplified expressions
\(75gd = \frac{1}{2}(5 \times 169 g - 180gd)\) M1
Use of \(F = \mu R\) and solve for \(d\)
\(150gd + 180gd = 845g, d = \frac{169}{66}\) A1
(= 2.6 m or better)
(4)
Question 5b alt t
Answer Marks
Guidance
\(R = 5g - \frac{12}{13}P, F = \frac{5}{13}P\) M1
Substitute trig in their equations from resolving.
\(\frac{5}{13}P = \frac{1}{2}\left(5g - \frac{12}{13}P\right)\) M1
use \(F = \mu R\) and solve for \(d\)
\(\Rightarrow P = \frac{65}{22}g\) A1
\(d = \frac{4P}{5g \cos \theta} = \frac{169}{66}\) A1
[12]
Question 6a
Answer Marks
Guidance
Horizontal motion: \(x = 3t\) B1
Vertical motion: \(y = 4t - \frac{g}{2}t^2\) M1
Correct use of suvat. Condone sign error(s)
A1
\(\left(y = 4 \times \frac{x}{3} - \frac{g}{2} \times \frac{x^2}{9}\right), \lambda = -\left(\frac{4 \times}{3} - \frac{gx^2}{18}\right)\) M1
Use \(y = -x\) and form an equation in one variable
\(\frac{7\lambda}{3} - \frac{g\lambda^2}{18}\) M1
solve for \(\lambda\)
\(\lambda = \frac{42}{g}\) or 4.3 (4.29) A1
(6)
Question 6a alt
Answer Marks
Guidance
Horizontal motion: \(x = 3t\) B1
Vertical motion: \(y = 4t - \frac{g}{2}t^2\) M1
Correct use of suvat. Condone sign error(s)
A1
\(\Rightarrow -3t = 4t - \frac{1}{2}gt^2, \left(t = \frac{14}{g}\right)\) M1
Use \(y = -x\) and form an equation in one variable
\(\lambda = 3t\) M1
Solve for \(\lambda\)
\(\lambda = 4.3\) (4.29) A1 (6)
Question 6b
Answer Marks
Guidance
At A: \(v \to 3 \text{ (m s}^{-1})\) B1
\(v \uparrow \quad 4 - g \times \frac{14}{g}\) M1
Complete method using suvat to find \(v \uparrow\) with their \(t\) or \(\lambda\)
\(= -10 \text{ (m s}^{-1})\) A1
Accept +10 with direction confirmed by diagram
Speed \(= \sqrt{(\text{their } 10)^2 + (3)^2}\) DM1
Dependent on the first M1 in (b)
\(= \sqrt{109 \text{ (m s}^{-1})\) A1
(10.4) Allow for \(v \uparrow = 10\)
\(\tan^{-1}\left(\frac{\text{their } 10}{3}\right)\) or \(\tan^{-1}\left(\frac{3}{\text{their } 10}\right)\) DM1
Use trig to find a relevant angle. Dependent on the first M1 in (b)
Direction \(= 73.3°\) below the horizontal A1
(1.28 radians) Accept direction \(3\mathbf{i} - 10\mathbf{j}\). Do not accept a bearing
(7)
Question 6b alt
Answer Marks
Guidance
Loss in GPE: \(mg \lambda A = 42m\) B1
Gain in KE: \(\frac{1}{2}mv^2 - \frac{1}{2}m \times 25\) M1
Terms must be dimensionally correct. Condone sign error.
Solve for v: \(42 = \frac{1}{2}v^2 - \frac{25}{2}\) M1
\(v = \sqrt{109}\) A1
\(v \cos \theta = 3\) M1
Use trig. to find a relevant angle
\(\theta = 73.3°\) below the horizontal A1 (7)
Accept correct angle marked correctly on a diagram.
[13]
Question 7a
Answer Marks
Guidance
CLM: \(6mu = 2mv + 3mw\) M1
Requires all 3 terms. Must be dimensionally correct. Condone sign error(s)
\((6u = 2v + 3w)\) A1
This equation defines their directions
Impact: \(w - v = \frac{3}{4} \times 3u \left(= \frac{9}{4}u\right)\) M1
Must be used with \(e\) on the correct side
A1 Penalise inconsistent directions here
\(6u = 2w - \frac{9}{2}u + 3w\) DM1
Solve simultaneous equations for \(v\) or \(w\). Dependent on the 2 previous M marks
\(w = \frac{21}{10}u = v_B\) A1
One correct
\(v = w - u = \left(\frac{21}{10} - \frac{9}{4}\right)u = -\frac{3}{20}u, v_A = -\frac{3}{20}u\) A1
Both correct
(7)
Question 7b
Answer Marks
Guidance
Speed of B after hitting wall = \(\frac{21}{10}ue\) M1(B1)
\(e \times\) their \(w\)
Impulse = \(\frac{27}{4}mu = 3m\left(\frac{21}{10}u + \frac{21}{10}ue\right)\) M1
for their \(w\). Must be trying to use the correct equation with \(3m\).
\(\frac{9}{4} \times \frac{10}{10}(1 + e), e = \frac{1}{14}\) A1
(3)
Question 7b alt
Answer Marks
Guidance
Impulse = \(\frac{27}{4}mu = 3m\left(\frac{21}{10} + V\right), \left(V = \frac{3u}{20}\right)\) M1(B1)
Use impulse to find \(V\). Must be trying to use the correct equation with \(3m\).
\(\frac{21u}{10} = e \times\) their \(w\). M1
\(V = e \times\) their \(w\).
\(e = \frac{1}{14}\) A1
(3)
Question 7c
Answer Marks
Guidance
Speed of B after second impact = \(\frac{1}{14} \times \frac{21}{10}u = \frac{3}{20}u\) B1 ft
Compare two relevant speeds. (ft on their \(V\) or their \(e \times\) their \(w\))
Same velocity (and A has a head start), so no collision. B1
From correct work only
(2) [12]
Copy
Since this question is about the magnitude of the impulse, condone subtraction in the "wrong order" throughout.
| $m\mathbf{v} - m\mathbf{u} = 0.6(2c\mathbf{i} - c\mathbf{j} - c\mathbf{i} - 2c\mathbf{j})$ | M1 | Impulse = change in momentum. Marking the RHS only |
| $= 0.6(c\mathbf{i} - 3c\mathbf{j})$ | A1 | |
| Magnitude $= 0.6\sqrt{c^2 + 9c^2}$ | DM1 | Correct use of Pythagoras' theorem on $m\mathbf{v} - m\mathbf{u}$ or $\mathbf{v} - \mathbf{u}$. Marking the RHS only. Dependent on the previous M1 |
| $= 0.6\sqrt{10c} = (-0.6\sqrt{10c^2})$ | A1 | Accept $\sqrt{10}c$ for change in velocity |
| The next two marks are not available to a candidate who has equated a scalar to a vector. | | |
| $2\sqrt{10} = 0.6\sqrt{10}c$ | DM1 | Equate & solve for $c$. Dependent on the previous M1 |
| $c = \frac{10}{3}$ | A1 | Accept 3.3 or better |
| | (6) | |
## Question 3 alt
| $m\mathbf{v} - m\mathbf{u} = 0.6(2c\mathbf{i} - c\mathbf{j} - c\mathbf{i} - 2c\mathbf{j})$ | M1 | change in momentum |
| $= 0.6(c\mathbf{i} - 3c\mathbf{j})$ | A1 | |
| Square of magnitude | DM1 | |
| $= 0.36(10c^2)$ | A1 | |
| The next two marks are not available to a candidate who has equated a scalar to a vector. | | |
| $40 = 0.36(c^2 + 9c^2)$ | DM1 | Equate & solve for $c$ |
| $c = \frac{10}{3}$ | A1 | |
| | (6) | |
## Question 3 alt (impulse momentum equation)
| $\begin{pmatrix} 2\sqrt{10} \cos \theta \\ 2\sqrt{10} \sin \theta \end{pmatrix} = 0.6 \begin{pmatrix} 2c - c \\ -c - 2c \end{pmatrix}$ | M1 | Impulse momentum equation |
| $= 0.6c \begin{pmatrix} 1 \\ -3 \end{pmatrix}$ | A1 | Correct equation |
| $2\sqrt{10} \cos \theta = 0.6c$ | DM1 | Compare coefficients and form equation for $\theta$ |
| $2\sqrt{10} \sin \theta = -3 \times 0.6c$ | | |
| $\tan \theta = -3 \Rightarrow \cos \theta = (\pm) \frac{1}{\sqrt{10}}$ | A1 | $\cos \theta$ or $\sin \theta$ correct |
| $2\sqrt{10} \cos \theta = 0.6c$ | DM1 | |
| $\Rightarrow c = \frac{10}{3}$ | A1 | |
## Question 3 alt (impulse momentum triangle)
| Impulse momentum triangle. Units used for the vectors must be dimensionally correct | M1 | |
| Sides of magnitude $\sqrt{5c}, \sqrt{5c}, \frac{10\sqrt{10}}{3}$ or $\frac{3\sqrt{5c}}{5}, \frac{3\sqrt{5c}}{5}, 2\sqrt{10}$ | A1 | |
| $\mathbf{u} \cdot \mathbf{v} = \begin{pmatrix} c \\ 2c \end{pmatrix} \cdot \begin{pmatrix} 2c \\ -c \end{pmatrix}$ | DM1 | Use of scalar product |
| $= 2c^2 - 2c^2 = 0 \therefore$ at $90°$ | A1 | ...to show velocities perpendicular. Use of Pythagoras' theorem in a right angled triangle |
| $(0.6 \times \sqrt{5c})^2 + (0.6 \times \sqrt{5c})^2 = (2\sqrt{10})^2$ | DM1 | |
| $\frac{18c^2}{5} = 40, c = \frac{10}{3}$ | A1 | |
| | (6) | |
## Question 4a
| | Triangle | sector |
|---|---|---|
| mass | 4.5 | $4\pi$ (= 12.56..) |
| c of m from O | $\frac{2}{3}, \frac{3\sqrt{2}}{2}$ (= 1.41...) | $\frac{16\sqrt{2}}{3\pi}$ (= 2.40....) |
| B1 | Mass ratios |
| B1 | Distances |
| | | Distances from $AD$ are $-\frac{1}{3} \times \frac{3\sqrt{2}}{2}$ and $\frac{16\sqrt{2}}{3\pi} - \frac{3\sqrt{2}}{2}$ (= 0.280) |
| $4\pi \times \frac{16\sqrt{2}}{3\pi} - 4.5\sqrt{2} = \left(\frac{101\sqrt{2}}{6}\right) = (4\pi - 4.5)d$ | M1 | Moments about an axis through O and parallel to DA. Terms must be dimensionally correct. Shapes combined correctly. |
| | A1 | Correct unsimplified equation |
| $d = \frac{101\sqrt{2}}{6(4\pi - 4.5)} = 2.951.....$ | | (distance from O) |
| Distance from $DA = 2.951... - \frac{3\sqrt{2}}{2} = 0.830 \text{ (0.83) m}$ | A1 | Accept $\frac{101\sqrt{2}}{6(4\pi - 4.5)} - \frac{3\sqrt{2}}{2}$ |
| | (5) | |
## Question 4a alt
| | Triangle | sector |
|---|---|---|
| mass | 4.5 | $4\pi (= 12.56..)$ |
| c of m from both axes $OC, OB$ | 1 | $\frac{16\sqrt{2}}{3\pi} \times \frac{1}{\sqrt{2}} = \frac{16}{3\pi}$ |
| $4\pi \times \frac{16}{3\pi} - 4.5 \times 1 = (4\pi - 4.5)\bar{x}$ | M1 | Moments about an axis through O. Terms must be dimensionally correct. Condone sign error(s) |
| $(\bar{x} = \bar{y} = \frac{101}{6(4\pi - 4.5)})$ | A1 | Correct unsimplified equation |
| $d = \frac{101\sqrt{2}}{6(4\pi - 4.5)}$ | | Distance from O |
| Distance from $DA = 2.951... - \frac{3\sqrt{2}}{2} = 0.830 \text{ (0.83) m}$ | A1 | |
| | (5) | |
## Question 4b
| $\tan \theta = \frac{\text{their } 0.830}{2.12}$ or $\tan \phi = \frac{2.12}{\text{their } 0.830}$ | M1 | Use of tan to find a relevant angle: |
| $21.4°$ or $68.6°$ | A1 | |
| Angle between DC and downward vertical = $135° -$ their $\theta$ | M1 | Correct method for the required angle |
| $= 114°$ | A1 | The Q asks for the angle to the nearest degree. |
| | (4) | |
## Question 4b alt
| $GD^2 = OD^2 + OG^2 - 2OD \cdot OG \cos 45$ | M1 | Complete method to find angle $ODG$ |
| $(GD = 2.28)$ | | |
| $\sin 45 = \frac{\sin \theta}{DG}$ and $\frac{\sin \theta}{OG}$ | | |
| $\Rightarrow \theta = 66.4°$ | A1 | |
| Required angle = $180° - 66.4° = 114°$ | M1 A1 | Correct method for the required angle. The Q asks for the angle to the nearest degree. |
| | (4) [9] | |
## Question 5a
| M(A): $d \cos \theta \times 5g = 4P$ | M1 | Terms must be dimensionally correct. Condone trig confusion |
| Resolving horizontally: $P \sin \theta = F$ | B1 | |
| Resolving vertically: $P \cos \theta + R = 5g$ | M1 | Requires all 3 terms. Condone trig confusion and sign errors |
| | A1 | Correct equation |
| | DM1 | Substitute for $P$ to find $R$ or $F$. Dependent on both previous M marks. One force correct. Accept equivalent forms e.g. $R = \frac{20g - 5gd + 20g \tan^2 \theta}{4(1 + \tan^2 \theta)}$ |
| $R = 5g - \frac{5gd \cos^2 \theta}{4}$ | A1 | One force correct |
| $F = \frac{5gd \cos \theta \sin \theta}{4}$ | A1 | Both forces correct. Accept equivalent forms e.g. $F = \frac{5gd \tan \theta}{4 \sec^2 \theta}$ |
| | (8) | |
## Question 5a alt
| M(B): | M1 | Needs all three terms. Terms must be dimensionally correct. Condone trig confusion |
| $5g \cos \theta \times (4 - d) + F \sin \theta \times 4 = R \cos \theta \times 4$ | | |
| Resolve parallel to the rod: | M1 | Requires all 3 terms. Condone trig confusion and sign errors |
| $5g \sin \theta = R \sin \theta + F \cos \theta$ | B1 | At most one error |
| | A1 | Correct equation |
| $\Rightarrow R = 5g - \frac{F \cos \theta}{\sin \theta}$ | | |
| $5g \cos \theta \times (4 - d) + F \sin \theta \times 4 = 4 \cos \theta \left(5g - \frac{F \cos \theta}{\sin \theta}\right)$ | DM1 | Eliminate one variable to find $F$ or $R$. Dependent on both previous M marks |
| $4F \left(\sin \theta + \frac{\cos^2 \theta}{\sin \theta}\right) = 20g \cos \theta - 20g \cos \theta + 5gd \cos \theta$ | | |
| $= 20g \cos \theta - 20g \cos \theta + 5gd \cos \theta$ | | |
| $F = \frac{5gd \cos \theta \sin \theta}{4}$ | A1 | One force correct |
| $R = 5g - \frac{5gd \cos^2 \theta}{4}$ | A1 | Both forces correct |
## Question 5b
| $\mu = \frac{\frac{5gd \cos \theta \sin \theta}{4}}{5g - \frac{5gd \cos^2 \theta}{4}}$ | M1 | Use of $F = \mu R$ |
| $\frac{1}{2}\left(5g - \frac{5gd \cos^2 \theta}{4}\right) = \frac{5gd \cos \theta \sin \theta}{4}$ | A1 | $(4 - d \cos^2 \theta = 2d \cos \theta \sin \theta)$ |
| $4 \times 169 - 120d + 144d$ | M1 | Use $\tan \theta = \frac{5}{12}$ and solve for $d$ |
| $d = \frac{169}{66}$ | A1 | (= 2.6 m or better) |
| | (4) | |
## Question 5b alt
| $F = 5gd \times \frac{12}{13} \times \frac{5}{13} \times \frac{1}{4} = \left(\frac{75gd}{169}\right)$ | M1 | Use $\tan \theta = \frac{5}{12}$ |
| $R = 5g - \frac{5gd}{4} \times \frac{144}{169}$ | A1 | Both unsimplified expressions |
| $75gd = \frac{1}{2}(5 \times 169 g - 180gd)$ | M1 | Use of $F = \mu R$ and solve for $d$ |
| $150gd + 180gd = 845g, d = \frac{169}{66}$ | A1 | (= 2.6 m or better) |
| | (4) | |
## Question 5b alt t
| $R = 5g - \frac{12}{13}P, F = \frac{5}{13}P$ | M1 | Substitute trig in their equations from resolving. |
| $\frac{5}{13}P = \frac{1}{2}\left(5g - \frac{12}{13}P\right)$ | M1 | use $F = \mu R$ and solve for $d$ |
| $\Rightarrow P = \frac{65}{22}g$ | A1 | |
| $d = \frac{4P}{5g \cos \theta} = \frac{169}{66}$ | A1 | |
| | [12] | |
## Question 6a
| Horizontal motion: $x = 3t$ | B1 | |
| Vertical motion: $y = 4t - \frac{g}{2}t^2$ | M1 | Correct use of suvat. Condone sign error(s) |
| | A1 | |
| $\left(y = 4 \times \frac{x}{3} - \frac{g}{2} \times \frac{x^2}{9}\right), \lambda = -\left(\frac{4 \times}{3} - \frac{gx^2}{18}\right)$ | M1 | Use $y = -x$ and form an equation in one variable |
| $\frac{7\lambda}{3} - \frac{g\lambda^2}{18}$ | M1 | solve for $\lambda$ |
| $\lambda = \frac{42}{g}$ or 4.3 (4.29) | A1 | (6) | Not $\frac{30}{7}$ |
## Question 6a alt
| Horizontal motion: $x = 3t$ | B1 | |
| Vertical motion: $y = 4t - \frac{g}{2}t^2$ | M1 | Correct use of suvat. Condone sign error(s) |
| | A1 | |
| $\Rightarrow -3t = 4t - \frac{1}{2}gt^2, \left(t = \frac{14}{g}\right)$ | M1 | Use $y = -x$ and form an equation in one variable |
| $\lambda = 3t$ | M1 | Solve for $\lambda$ |
| $\lambda = 4.3$ (4.29) | A1 (6) | |
## Question 6b
| At A: $v \to 3 \text{ (m s}^{-1})$ | B1 | |
| $v \uparrow \quad 4 - g \times \frac{14}{g}$ | M1 | Complete method using suvat to find $v \uparrow$ with their $t$ or $\lambda$ |
| | | $= -10 \text{ (m s}^{-1})$ | A1 | Accept +10 with direction confirmed by diagram |
| Speed $= \sqrt{(\text{their } 10)^2 + (3)^2}$ | DM1 | Dependent on the first M1 in (b) |
| $= \sqrt{109 \text{ (m s}^{-1})$ | A1 | (10.4) Allow for $v \uparrow = 10$ |
| $\tan^{-1}\left(\frac{\text{their } 10}{3}\right)$ or $\tan^{-1}\left(\frac{3}{\text{their } 10}\right)$ | DM1 | Use trig to find a relevant angle. Dependent on the first M1 in (b) |
| Direction $= 73.3°$ below the horizontal | A1 | (1.28 radians) Accept direction $3\mathbf{i} - 10\mathbf{j}$. Do not accept a bearing |
| | (7) | |
## Question 6b alt
| Loss in GPE: $mg \lambda A = 42m$ | B1 | |
| Gain in KE: $\frac{1}{2}mv^2 - \frac{1}{2}m \times 25$ | M1 | Terms must be dimensionally correct. Condone sign error. |
| Solve for v: $42 = \frac{1}{2}v^2 - \frac{25}{2}$ | M1 | |
| $v = \sqrt{109}$ | A1 | |
| $v \cos \theta = 3$ | M1 | Use trig. to find a relevant angle |
| $\theta = 73.3°$ below the horizontal | A1 (7) | Accept correct angle marked correctly on a diagram. |
| | [13] | |
## Question 7a
| CLM: $6mu = 2mv + 3mw$ | M1 | Requires all 3 terms. Must be dimensionally correct. Condone sign error(s) |
| $(6u = 2v + 3w)$ | A1 | This equation defines their directions |
| Impact: $w - v = \frac{3}{4} \times 3u \left(= \frac{9}{4}u\right)$ | M1 | Must be used with $e$ on the correct side |
| | A1 | Penalise inconsistent directions here |
| $6u = 2w - \frac{9}{2}u + 3w$ | DM1 | Solve simultaneous equations for $v$ or $w$. Dependent on the 2 previous M marks |
| $w = \frac{21}{10}u = v_B$ | A1 | One correct |
| $v = w - u = \left(\frac{21}{10} - \frac{9}{4}\right)u = -\frac{3}{20}u, v_A = -\frac{3}{20}u$ | A1 | Both correct |
| | (7) | |
## Question 7b
| Speed of B after hitting wall = $\frac{21}{10}ue$ | M1(B1) | $e \times$ their $w$ |
| Impulse = $\frac{27}{4}mu = 3m\left(\frac{21}{10}u + \frac{21}{10}ue\right)$ | M1 | for their $w$. Must be trying to use the correct equation with $3m$. |
| $\frac{9}{4} \times \frac{10}{10}(1 + e), e = \frac{1}{14}$ | A1 | (3) |
## Question 7b alt
| Impulse = $\frac{27}{4}mu = 3m\left(\frac{21}{10} + V\right), \left(V = \frac{3u}{20}\right)$ | M1(B1) | Use impulse to find $V$. Must be trying to use the correct equation with $3m$. |
| $\frac{21u}{10} = e \times$ their $w$. | M1 | $V = e \times$ their $w$. |
| $e = \frac{1}{14}$ | A1 | (3) |
## Question 7c
| Speed of B after second impact = $\frac{1}{14} \times \frac{21}{10}u = \frac{3}{20}u$ | B1 ft | Compare two relevant speeds. (ft on their $V$ or their $e \times$ their $w$) |
| Same velocity (and A has a head start), so no collision. | B1 | From correct work only |
| | (2) [12] | |
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3. A particle of mass 0.6 kg is moving with constant velocity ( $c \mathbf { i } + 2 c \mathbf { j }$ ) $\mathrm { ms } ^ { - 1 }$, where $c$ is a positive constant. The particle receives an impulse of magnitude $2 \sqrt { 10 } \mathrm {~N} \mathrm {~s}$. Immediately after receiving the impulse the particle has velocity ( $2 c \mathbf { i } - c \mathbf { j }$ ) $\mathrm { ms } ^ { - 1 }$.
Find the value of $c$.\\
(6)\\
\hfill \mbox{\textit{Edexcel M2 2016 Q3 [6]}}