Answer:
[tex]W_f =4.7968 rad/s[/tex]
Explanation:
By the law of the conservation of the angular momentum L:
[tex]L_i = L_f[/tex]
Where:
[tex]L_i=I_iW_i[/tex]
[tex]L_f=I_fW_f[/tex]
where [tex]I_i[/tex] is the inicial moment of inertia, [tex]W_i[/tex] is the initial angular velocity, [tex]I_f[/tex] is the final moment of inertia and [tex]W_f[/tex] is the final angular velocity.
Replacing:
[tex]I_iW_i = I_fW_f[/tex]
Now, we have to change the angular velocity from revolutions to radians as:
[tex]W_i=0.3*2\pi rad/s[/tex]
[tex]W_i=1.884 rad/s[/tex]
Then, we find the initial moment of inertia ([tex]I_i[/tex]) as:
[tex]I_i = \frac{1}{12}(M)(R_1)^2+0.4[/tex]
[tex]I_i = \frac{1}{12}(9 kg)(1.7m)^2+0.4[/tex]
[tex]I_i = 2.5675 kg*m^2[/tex]
Where M is the mass of his hands and arms and R1 is the length of his arms and hands whe they are outstretched.
Now we find the final moment of inertia ([tex]I_f[/tex]) as:
[tex]I_f = MR_2^2+0.4[/tex]
[tex]I_f = (9)(0.26)^2+0.4[/tex]
[tex]I_ f = 1.0084 kg*m^2[/tex]
Where R2 is the radius of the cylinder formed.
Finally we replace all in the first equation as:
[tex]I_iW_i = I_fW_f[/tex]
[tex](2.5675)(1.884) = (1.0084)W_f[/tex]
Solving for [tex]W_f[/tex], we get:
[tex]W_f =4.7968 rad/s[/tex]