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For a particle in uniform circular motion, the acceleration a at a point P(R,θ) on the circle of radius R is (Here θ is measured with the x-axis)
- -(v²)/(R)cosθ î + (v²)/(R)sinθ ĵ
- -(v²)/(R)sinθ î + (v²)/(R)cosθ ĵ
- -(v²)/(R)cosθ î - (v²)/(R)sinθ ĵ
- (v²)/(R)î + (v²)/(R)ĵ
Correct answer: -(v²)/(R)cosθ î - (v²)/(R)sinθ ĵ
Solution
In uniform circular motion the acceleration is purely centripetal, directed from P(R,theta) toward the center, i.e. opposite the radial unit vector (cos theta i + sin theta j). Hence a = -(v^2/R)cos theta i - (v^2/R)sin theta j.
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