Question 32898
Let us first write parametric equations for uniform circular motion.
x ( t ) = R cos ( ω t ) ; y ( t ) = R sin ( ω t ) . x(t) = R \cos(\omega t); \quad y(t) = R \sin(\omega t). x ( t ) = R cos ( ω t ) ; y ( t ) = R sin ( ω t ) .
The x and y projections of velocity are:
v x = x ′ ( t ) = − R ω sin ( ω t ) ; v y = y ′ ( t ) = R ω cos ( ω t ) . v_x = x'(t) = -R\omega \sin(\omega t); \quad v_y = y'(t) = R\omega \cos(\omega t). v x = x ′ ( t ) = − R ω sin ( ω t ) ; v y = y ′ ( t ) = R ω cos ( ω t ) .
The absolute value of velocity is v = v x 2 + v y 2 = ω R v = \sqrt{v_x^2 + v_y^2} = \omega R v = v x 2 + v y 2 = ω R .
The x and y projections of acceleration are:
a x = x ′ ′ ( t ) = − R ω 2 cos ( ω t ) ; a y = y ′ ′ ( t ) = − R ω 2 sin ( ω t ) . a_x = x''(t) = -R\omega^2 \cos(\omega t); \quad a_y = y''(t) = -R\omega^2 \sin(\omega t). a x = x ′′ ( t ) = − R ω 2 cos ( ω t ) ; a y = y ′′ ( t ) = − R ω 2 sin ( ω t ) .
Therefore, absolute value of acceleration is a = a x 2 + a y 2 = ω 2 R a = \sqrt{a_x^2 + a_y^2} = \omega^2 R a = a x 2 + a y 2 = ω 2 R , or using expression for velocity,
a = v 2 R . a = \frac{v^2}{R}. a = R v 2 .