Here,
Motion of solid can be imagined to be in pure rotation about a point (say I) at a certain Instant. The instantaneous axis whose positive sense is directer ding w of the solid and which passes through the point I is Instantaneous axis of Rotation.
velocity vector of an point (P) of the solid
is →Vp=→W×→rPL...........(1)
on the basis of eq (1) for the (M.Cc)
of the disc:-
→Vc=→W×→rd............(2)
According to the given problem : →Vc↑i
and →w↑↑^x i,e →w⊥x−y plane, so to satisfy the Eqn (2), →rC is directed along (→−j). Hence point I is at distance →rcy=y
Using above : equation (2) becomes:-
Vc=wy or y=vCw..........(3)
(b) From the angular kinematics Equation:-
W2=WO2+β2t(β2 is acc along axis)
w=|3tbx|
on other hande, x=vt (where 'x' is the ordinate of the O.M)
∴t=xv...........(5)
From (4) and (5) cv=βxv
From (3)
and y=vcw=vβx/v=v2βx (Hyper bola)
Given
β=α
∴y=v2αx
(a) and As centre ′C′ moves with constant acceleration (a), with
zero initial velocity:-
x=at2 and vc=at
∴Vc=a√2xa=√2xa
Hence y=vcw=2xw