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How do you get this v = MT ∗ m^−1 ∗ 2^1/2 ∗ g^1/2 ∗ R^1/2cm ∗ (1 − cos θ)^1/2 from this v =MT/m sqrt 2gRcm (1 − cos θ)?
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They're equivalent expressions \[\sqrt A = A^{1/2}\] \[\frac{1}{A} = A^{-1}\] so \[v=\frac{MT}{m} \sqrt{ 2gR_{cm} (1 − cos θ)}\] \[= MTm^{-1}\sqrt{ 2gR_{cm} (1 − cos θ)}\] \[= MTm^{-1}\Big(2gR_{cm} (1 − cos θ)\Big)^{1/2}\] \[=MTm^{-1} 2^{1/2} g^{1/2} R_{cm}^{1/2} (1-cos\theta)^{1/2}\]
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