The paper includes a full answer scheme at the end. Time allowed: 45 minutes Total marks: 36
At ( t = 1 ), ( v = 5 \ \text{m/s} ), ( s = 3 \ \text{m} ).
(b) ( s(t) = \int (8t^{3/2} - 54) dt = 8 \cdot \frac{2}{5} t^{5/2} - 54t + D = \frac{16}{5} t^{5/2} - 54t + D ) ( s(4) = \frac{16}{5} \cdot 32 - 216 + D = \frac{512}{5} - 216 + D = 20 ) ( \frac{512}{5} - 216 = \frac{512}{5} - \frac{1080}{5} = -\frac{568}{5} ) So ( -\frac{568}{5} + D = 20 \Rightarrow D = 20 + \frac{568}{5} = \frac{100}{5} + \frac{568}{5} = \frac{668}{5} ) [ s(t) = \frac{16}{5}t^{5/2} - 54t + \frac{668}{5} ] (a) ( v(t) = \int \left(3t - \frac{t^2}{2}\right) dt = \frac{3t^2}{2} - \frac{t^3}{6} + C ) Starts from rest: ( v(0) = 0 \Rightarrow C = 0 ) [ v(t) = \frac{3t^2}{2} - \frac{t^3}{6} ]
(a) Find the velocity function ( v(t) ) (2 marks) (b) Find the time when the car is momentarily at rest again (2 marks) (c) Find the distance travelled up to that time (1 mark) A particle’s acceleration is given by [ a(t) = 2\cos(2t) - \sin t ] At ( t = 0 ), ( v = 1 ), ( s = 0 ).
(b) ( s(t) = \int (\sin 2t + \cos t) dt = -\frac{1}{2}\cos 2t + \sin t + D ) ( s(0) = -\frac12(1) + 0 + D = -\frac12 + D = 0 \Rightarrow D = \frac12 ) [ s(t) = -\frac12\cos 2t + \sin t + \frac12 ] (a) ( v(t) = \int (12t^2 - 8t + 2) dt = 4t^3 - 4t^2 + 2t + C ) ( v(1) = 4 - 4 + 2 + C = 2 + C = 5 \Rightarrow C = 3 ) [ v(t) = 4t^3 - 4t^2 + 2t + 3 ]
(c) ( s(3) = 27 - 18 + 15 + 2 = 26 \ \text{m} ) (a) ( v(t) = \int 4(t+1)^{-2} dt = -4(t+1)^{-1} + C ) ( v(0) = -4 + C = 2 \Rightarrow C = 6 ) [ v(t) = 6 - \frac{4}{t+1} ]