The total kinetic energy of the ball is the sum of the linear kinetic energy and angular kinetic energy:
"K_{tot} = K_{linear}+K_{angular}".
By definition:
"K_{linear} = \\dfrac12mv^2; \\space K_{angular} = \\dfrac12I\\omega^2" ,
where "m" is body mass, "v" - linear velocity, "I" - moment of inertia around the axis of rotation, "\\omega" - angular rotational frequency.
The moment of inertia of the ball is "I = \\dfrac{1}{10}md^2" , where "d" is the diameter of the ball.
Putting it all together in the first expression, obtain:
"K_{tot} =\\dfrac12mv^2+ \\dfrac12\\dfrac{1}{10}md^2\\omega^2" .
Express "\\omega" and substitute numerical values:
"\\omega^2 =\\dfrac{ 20(K_{tot}- \\dfrac12mv^2)}{md^2}=\\dfrac{ 20(67.67- 0.5\\cdot 0.0459\\cdot 54.15^2)}{0.0459\\cdot 0.0426^2} = 90157" .
Thus, "\\omega = \\sqrt{90157} \\approx300" rad/s
The rotational frequency in rpm is:
"f = 60\\cdot\\dfrac{\\omega}{2\\pi} = 2864.8" rpm.
Answer. 2864.8 rpm.
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