Nomenclature is like this
u1xi = initial speed of moving ball in x-direction
u2xi = initial speed of stationary ball in x-direction
u1yi = initial speed of moving ball in y-direction
u2yi = initial speed of stationary ball in y-direction
V1 = final speed of initially moving ball
V2 = final speed of initially stationary ball
In a perfectly elastic collision
Suppose final velocity of stationary billiard ball is v2 and
it's making angle
with horizontal
axis
Using momentum conservation in x direction,
Pi = Pf
m1*u1xi + m2*u2xi = m1*V1x + m2*V2x
given that m1 = m & m2 = m
u1xi = 3 m/sec & u2xi = 0 (since stationary)
V1x = V1*cos 30 deg & V2 = V2*cos 
m*u1xi + m*u2xi = m*V1*cos(30 deg) + m*V2*cos 
u1xi + u2xi = V1*cos(30 deg) + V2*cos 
3 - 0 = V1*cos(30 deg) + V2*cos 
V1*cos(30 deg) + V2*cos
= 3
V2*cos
= 3 - V1*cos 30
deg
Using momentum conservation in y direction,
Pi = Pf
m1*u1yi + m2*u2yi = m1*V1y + m2*V2y
given that m1 = m & m2 = m
u1yi = 0 m/sec & u2yi = 0 m/sec
V1y = V1*sin 30 deg & V2y = -V2*sin 
m*u1i + m*u2i = m*V1*sin(30 deg) - m*V2*sin 
u1i + u2i = V1*sin(30 deg) - V2*sin 
0 - 0 = V1*sin(30 deg) - V2*sin 
V1*sin(30 deg) = V2*sin 
V2*sin
= (1/2)*V1
Now square and add both equation
V2^2*(sin2
+
cos2
) = (1/4)*V1^2 +
9 + (3/4)*V1^2 - (3*sqrt 3)*V1
V2^2*(1) = (1/4)*V1^2 + 9 + (3/4)*V1^2 - (3*sqrt 3)*V1
V2^2 = (1/4)*V1^2 + 9 + (3/4)*V1^2 - (3*sqrt 3)*V1
V2^2 = V1^2 + 9 - (3*sqrt 3)*V1
Now Using energy conservation in elastic collision
KEi = KEf
0.5*m*u1^2 + 0.5*m*u2^2 = 0.5*m*V1^2 +0.5*m*V2^2
u1^2 + u2^2 = V1^2 + V2^2
V1^2 + V2^2 = 3^2 + 0
V1^2 + V2^2 = 9
V2^2 = 9 - V1^2
Using above expression
9 - V1^2 = V1^2 + 9 - (3*sqrt 3)*V1
2*V1^2 - (3*sqrt 3)*V1 = 0
V1 = (3*sqrt 3)/2
V1 = 2.598 m/sec = 2.6 m/sec
So,
V2 = sqrt (9 - V1^2)
V2 = sqrt (9 - 2.598^2)
V2 = 1.50 m/sec = final speed of stationary billiard ball
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