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Further kinematics

Position is a vector. Differentiate it.

In a plane, a particle needs two numbers to say where it is. Write them as one vector in tt, and the calculus of Year 1 gives its velocity and acceleration, one component at a time.

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A vector in t

A particle moves so that after tt seconds

r=(t3−3t)i+(2t2−8t)j\mathbf{r} = (t^3 - 3t)\mathbf{i} + (2t^2 - 8t)\mathbf{j}

metres from OO, with i\mathbf{i} east and j\mathbf{j} north. The arrow riding with it is its velocity: always along the path.

Due south

At t=1t = 1 the velocity arrow points straight down the page: the particle is moving due south, parallel to j\mathbf{j}, at 4 m s⁻¹. Its i\mathbf{i}-component is zero.

Due east

At t=2t = 2 the other component vanishes:

v=9i\mathbf{v} = 9\mathbf{i}

so the particle is moving due east at 9 m s⁻¹, at the bottom of its dip.

The acceleration

Differentiate once more: a=6t i+4j\mathbf{a} = 6t\,\mathbf{i} + 4\mathbf{j}, shown dashed. It says which way the velocity is changing, and the velocity arrow keeps turning towards it: at t=2t = 2, a=12i+4j\mathbf{a} = 12\mathbf{i} + 4\mathbf{j}.

Chapter 5

Differentiate each component. Integrate back.

Constant acceleration as vectors, ships that meet, integrating with a vector constant, projectiles as vectors, and twelve graded exam questions with full worked solutions are waiting.