One end of a rod of length is located at coordinates . The other end is attached to a particle of mass . The rod makes an angle (in radians) with the horizontal.
At a particular instant, the state of the system is as follows:
What is the kinetic energy of the particle?
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First, we know that x = L cos θ and y = L sin θ
With some differentiation with respect to time, x ˙ = − L sin θ θ ˙ and y ˙ = L cos θ θ ˙
But let's not forget the initial conditions. So:
x ˙ = 1 − L sin θ θ ˙
y ˙ = 1 + L cos θ θ ˙
Where θ ˙ = − 1 and θ = 3 π
The square of the speed v 2 = 2 + 2 l ( sin θ − cos θ ) + L 2 ; this is just algebra.
Substituting values, we get E = 2 2 + 3