a)
Let the mass of the ball be m, radius of the ball be R , angular velocity be "\\omega"
Angular momentum,
"v=r\\times\\omega"
So, it is holonomic constraint.
b)
It is an example of scleronomic constraint.
"\\overrightarrow{r}=l\\theta"
c)
As bead is freely can move along the rod and the rod is also rotating in xy plane,
So,
"(x-h)^2+(y-k)^2=l^2"
So, it is non-holonomic motion.
d)
Bead can move over along the straight wire,
"v=g\\cos\\theta t"
"\\overrightarrow{r}=\\frac{g\\cos\\theta t^2}{2}"
"r^2-a^2>0"
Hence, it is a non-holonomic constraint.
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