The moment of inertia can be given as the sum of the moments of inertia of each of the end cylinders plus the moment of inertia of the axle is[tex]{a_y = \frac{g}{1+\frac{R^2}{2r^2}}}[/tex]
Imagine the YoYo When yoyo is falling
In Linear downward direction,
mg-T=ma_y
ay = is linear acceleration
now
[tex]T*r=I_c_m \alpha[/tex]
but from we also know [tex]\alpha =\frac{a_y}{r}[/tex]
[tex]T*r=I_c_m \frac{a_y}{r}[/tex]
substiting above equation in beggining eqyation.
[tex]mg-I_c_m \frac{a_y}{r^2} = ma_y[/tex]
[tex]a_y = \frac{mg}{m+\frac{I_c_m}{r^2}} .......................(1)[/tex]
Icm --> The moment of inertia can be given as the sum of the moments of inertia of each of the end cylinders plus the moment of inertia of the axle:
and mass ofcylinders will half of total mass as spindle mass is negigible. i.e cylinders masses = m/2
[tex]I_c_m =2* \frac{\frac{m}{2}R^2}{2} = \frac{mR^2}{2}...............(2)[/tex]
Substituting 2 in 1 we get
[tex]{ a_y = \frac{g}{1+\frac{R^2}{2r^2}}}[/tex]
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