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SUVAT in 2D Simplified Revision Notes

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2.5.1 SUVAT in 2D

Vectors in Kinematics

The SUVAT equations can be extended to two dimensions. However, strictly speaking, there is no such thing as "squared" vectors, so any equations with squared vector quantities are invalid.

Kinematics Equations:

  • Motion in a straight line (1D):
  • v=u+atv = u + at
  • s=ut+12at2s = ut + \frac{1}{2}at^2
  • s=12(u+v)ts = \frac{1}{2}(u+v)t
  • v2=u2+2asv^2 = u^2 + 2as
  • s=vt12at2s = vt - \frac{1}{2}at^2
  • Motion in two dimensions (2D):
  • v=u+at\mathbf{v} = \mathbf{u} + \mathbf{a}t
  • s=ut+12at2\mathbf{s} = \mathbf{u}t + \frac{1}{2}\mathbf{a}t^2
  • s=12(u+v)t\mathbf{s} = \frac{1}{2}(\mathbf{u}+\mathbf{v})t
  • s=vt12at2\mathbf{s} = \mathbf{v}t - \frac{1}{2}\mathbf{a}t^2

Problem Statement:

infoNote

A particle starts from the point with position vector (3i+7j)(3\mathbf{i} + 7\mathbf{j}) m and moves with constant velocity (2ij)ms1(2\mathbf{i} - \mathbf{j}) m s^{-1}. a) Find the position vector of the particle 4 seconds later.

b) Find the time at which the particle is due east of the origin.

Solution:

Given:

  • Initial position vector s0=(3,7)\mathbf{s_0} = (3, 7)
  • Velocity vector u=v=(2,1)\mathbf{u} = \mathbf{v} = (2, -1) (since velocity is constant)
  • Acceleration vector a=(0,0)\mathbf{a} = (0, 0)
  • Time t=4t = 4

Part (a):

To find the position vector s\mathbf{s}:

s=ut+12at2s=(2,1)(4)+12(0,0)(4)2=(8,4)\mathbf{s} = \mathbf{ut} + \frac{1}{2}\mathbf{a}t^2 \Rightarrow \mathbf{s} = \left(2, -1\right)(4) + \frac{1}{2}\left(0, 0\right)(4)^2 = \left(8, -4\right)

Remember, we didn't start at (0,00, 0):

Position=(3,7)+(8,4)=(11,3)\text{Position} = \left(3, 7\right) + \left(8, -4\right) = \left(11, 3\right)

Part (b):

  • Context: Due east means y=0y = 0 and xx has a value, say kk. image

In part (a), we worked out a position from a known time. We must adapt this method for an unknown time, t.

Equation:

r=Initial Position+Displacement\mathbf{r} = \text{Initial Position} + \text{Displacement} r=(37)+(21)t+12(00)t2=(3+2t7t) m\mathbf{r} = \left( \begin{array}{c} 3 \\ 7 \end{array} \right) + \left( \begin{array}{c} 2 \\ -1 \end{array} \right)t + \frac{1}{2} \left( \begin{array}{c} 0 \\ 0 \end{array} \right)t^2 = \left( \begin{array}{c} 3 + 2t \\ 7 - t \end{array} \right) \text{ m}
  • Since y=0y = 0, we set:
7t=0t=:highlight[7 seconds]7 - t = 0 \Rightarrow t = :highlight[7 \text{ seconds}]

Additional Problem:

infoNote

A particle P has velocity (3i+j)ms1)(-3\mathbf{i} + \mathbf{j}) m s^{-1}) at time t=0t = 0. The particle moves with constant acceleration a=(2i+3j)ms2\mathbf{a} = (2\mathbf{i} + 3\mathbf{j}) m s^{-2}. Find the speed of the particle and the bearing on which it is traveling at time t=3t = 3 seconds.

Given:

  • s=?\mathbf{s} = ?
  • u=(3,1)\mathbf{u} = \left( -3, 1 \right)
  • v=?\mathbf{v} = ?
  • a=(2,3)\mathbf{a} = \left( 2, 3 \right)
  • t=3t = 3 Velocity:
v=u+at\mathbf{v} = \mathbf{u} + \mathbf{a}t r=(31)+(23)(3)=(3+61+9)=(310)\mathbf{r} = \left( \begin{array}{c} -3 \\ 1 \end{array} \right) + \left( \begin{array}{c} 2 \\ 3 \end{array} \right)^{(3)}= \left( \begin{array}{c} -3 + 6 \\ 1 + 9 \end{array} \right)=\left( \begin{array}{c} 3 \\ 10 \end{array} \right)
  • Magnitude of velocity:
v=32+102=:highlight[109 m s1]|\mathbf{v}| = \sqrt{3^2 + 10^2} = :highlight[\sqrt{109} \text{ m s\(^{-1}\)}] image

Bearing:

tanθ=103θ=73.301\tan \theta = \frac{10}{3} \Rightarrow \theta = 73.301^\circ
  • Final Bearing:
Bearing=:highlight[16.7]\therefore \text{Bearing} = :highlight[16.7^\circ]

Problem: Ice Skater on an Ice Rink

infoNote

An ice skater is skating on a large flat ice rink. At time t=0t = 0, the skater is at a fixed point O and is traveling with velocity (2.4i0.6j)ms1)(2.4\mathbf{i} - 0.6\mathbf{j}) m s^{-1}). At time t=20t = 20 s, the skater is traveling with velocity (5.6i+3.4j)ms1(-5.6\mathbf{i} + 3.4\mathbf{j}) ms^{-1}.

Relative to OO, the skater has position vector s\mathbf{s} at time tt seconds.

Modelling the ice skater as a particle with constant acceleration, find:

a) The acceleration of the ice skater.

b) An expression for s\mathbf{s} in terms of tt.

c) The time at which the skater is directly north-east of OO.

A second skater travels so that she has position vector r=(1.1t6j) \mathbf{r} = (1.1t - 6\mathbf{j}) m relative to OO at time tt.

d) Show that the two skaters will meet.


Solution:

Part (a): Acceleration of the Ice Skater

Given:

  • Initial velocity u=(2.40.6)\mathbf{u} = \left( \begin{array}{c} 2.4 \\ -0.6 \end{array} \right)
  • Final velocity v=(5.63.4)\mathbf{v} = \left( \begin{array}{c} -5.6 \\ 3.4 \end{array} \right)
  • a=?\mathbf{a}=?
  • Time t=20st = 20 s Using the equation v=u+at\mathbf{v} = \mathbf{u} + \mathbf{a}t:
(5.63.4)=(2.40.6)+a(20)\left( \begin{array}{c} -5.6 \\ 3.4 \end{array} \right) = \left( \begin{array}{c} 2.4 \\ -0.6 \end{array} \right) + \mathbf{a}(20) (84)=20a\Rightarrow \left( \begin{array}{c} -8 \\ 4 \end{array} \right) = 20\mathbf{a} a=:success[(0.40.2) ms2]\Rightarrow \mathbf{a} = :success[\left( \begin{array}{c} -0.4 \\ 0.2 \end{array} \right) \text{ ms\(^{-2}\)}]

Part (b): Expression for s\mathbf{s} in terms of tt

Using the equation s=ut+12at2\mathbf{s} = \mathbf{ut} + \frac{1}{2}\mathbf{a}t^2:

s=(2.40.6)t+12(0.40.2)t2=(2.4t0.2t20.6t+0.1t2)\mathbf{s} = \left( \begin{array}{c} 2.4 \\ -0.6 \end{array} \right)t + \frac{1}{2}\left( \begin{array}{c} -0.4 \\ 0.2 \end{array} \right)t^2= \left( \begin{array}{c} 2.4t-0.2t^2 \\ -0.6t+0.1t^2 \end{array} \right) s=:success[(2.4t0.2t20.6t+0.1t2) m]\Rightarrow \mathbf{s} = :success[\left( \begin{array}{c} 2.4t-0.2t^2 \\ -0.6t+0.1t^2 \end{array} \right) \text{ m}]

Part (c): Time at which the skater is directly north-east of OO

North-east means the x-coordinate equals the y-coordinate, i.e., 2.4t0.2t2=0.6t+0.1t22.4t - 0.2t^2 = -0.6t + 0.1t^2:

2.4t0.2t2=0.6t+0.1t22.4t - 0.2t^2 = -0.6t + 0.1t^2 0.3t23t=0\Rightarrow 0.3t^2 - 3t = 0 image t(0.3t3)=00.3t=3t=:highlight[10 s]\Rightarrow t(0.3t - 3) = 0 \Rightarrow 0.3t = 3 \Rightarrow t = :highlight[10 \text{ s}]

Part (d): Show that the two skaters will meet

For the skaters to meet, their position vectors must be equal at the same time.

Given:

r1=(2.4t0.2t20.6t+0.1t2)\mathbf{r_1} = \left( \begin{array}{c} 2.4t-0.2t^2 \\ -0.6t+0.1t^2 \end{array} \right) r2=(01.1t6)\mathbf{r_2} = \left( \begin{array}{c} 0 \\ 1.1t-6 \end{array} \right)

To determine when the skaters meet, we need to find the time when the x-coordinates are equal:

Time when x-coordinates are equal:

2.4t0.2t2=02.4t - 0.2t^2 = 0

t(2.40.2t)=0\Rightarrow t(2.4 - 0.2t) = 0

2.4=0.2tt=:highlight[12 s]\Rightarrow 2.4 = 0.2t \Rightarrow t = :highlight[12 \text{ s}]

Now, check whether this time gives equal y-coordinates:

At t=12st = 12 s:

  • y-coordinate of skater 1: y1=0.6(12)+0.1(12)2=7.2y_1 = -0.6(12) + 0.1(12)^2 = 7.2

  • y-coordinate of skater 2: y2=1.1(12)6=7.2y_2 = 1.1(12) - 6 = 7.2

Since both y-coordinates are equal at t=12st = 12 s, the skaters meet at the position (07.2)m\left( \begin{array}{c} 0 \\ 7.2 \end{array} \right)m at t=12s.t = 12 s.


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