A torque τ acting through an angle ∆θ does a work W is given by the equation
W = -τ∆θ
The kinemativ equation of angular velocity and angular acceleration is given by the equation
"\u03c9^2=\u03c9_0^2 + 2\u03b1\u2206\u03b8"
The wheel angular acceleration can be found using the kinematics equation as
"\u03b1 = \\frac{\u03c9^2-\u03c9_0^2}{2\u2206\u03b8}"
"\u03c9_0" is initial angular speed and ω is final angular speed and ∆θ is angular displacement.
Since wheel come to rest after rotating through ¾ or 0.75 of a turn, its final angular velocity becomes zero (ω = 0).
In each turn wheel rotates 2π rad hence the total change in displacement after come to rest can be expressed as
"\u2206\u03b8 = (0.75)(\\frac{2\u03c0 \\;rad}{rev})"
Consider the wheel has a form of disk then moment of inertia of disk is given by the equation
"I = \\frac{1}{2}mr^2"
The relation between torque and moment of inertia can be expressed as
"\u03c4 = I\u03b1"
Here negative sign indicates torque exerted on the wheel to stop
"\u03c4 = (\\frac{1}{2}mr^2)(\\frac{\u03c9^2-\u03c9_0^2}{2\u2206\u03b8})"
"\u03c4 = -\\frac{1}{4}(\\frac{mr^2\u03c9_0^2}{\u2206\u03b8})"
Substitute 6.5 kg for mass of the disk (m), 0.7 m for radius of the disk (r), 1.5 rad/s for "\u03c9_0" and (0.75)"(\\frac{2\u03c0 \\;rad}{rev})" for ∆θ in the above equation and solve for torque.
"\u03c4 = -\\frac{1}{4}(\\frac{(6.5\\;kg)(0.7\\;m)^2(1.5 \\;rad\/s)^2}{0.75(2\u03c0 \\;rad\/rev)})"
"\u03c4 = -\\frac{1}{4} (1.52\\;N m)"
"\u03c4 = 0.38\\;N m"
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