Given: N_{ BO 1}=40 \text { r.p.m. or } \omega_{ BO 1}=2 \pi \times 40 / 60=4.2 rad / s
Since the length of crank O_{1} B=300 mm =0.3 m,therefore velocity of B with respect to O_{1} or simply velocity of B (because O_{1} is a fixed point),
v_{ BO 1}=v_{ B }=\omega_{ BO 1} \times O_{1} B=4.2 \times 0.3=1.26 m / s \ldots \text { (Perpendicular to } \left.O_{1} B\right)
1. Velocity of the ram R
First of all draw the space diagram, to some suitable scale, as shown in Fig.(a). Now the velocity diagram, as shown in Fig.(b), is drawn as discussed below :
1. Since O_{1} \text { and } O_{2} are fixed points, therefore these points are marked as one point in the velocity diagram. Draw vector o_{1} b perpendicular to O_{1} b, to some suitable scale, to represent the velocity of B with respect to O_{1} or simply velocity of B, such that
\text { vector } o_{1} b=v_{ BOl }=v_{ B }=1.26 m / s
2. From point o_{2} , draw vector o_{2} c perpendicular to O_{2} c to represent the velocity of the coincident point C with respect to O_{2} or simply velocity of C (i.e. v_{ CO 2} \text { or } v_{ C } ), and from point b, draw vector bc parallel to the path of motion of the sliding block (which is along the link O _{2} D) to represent the velocity of C with respect to B (i.e. v_{ CB }). The vectors O _{2} c and bc intersect at c.
3. Since the point D lies on O_{2} C produced, therefore divide the vector o_{2} cat d in the same ratio as D divides O_{2} C in the space diagram. In other words,
cd / o _{2} d = CD / O _{2} D
4. Now from point d, draw vector dr perpendicular to DR to represent the velocity of R with respect to D (i.e. v_{ RD } ), and from point o_{1} draw vector O_{1} r parallel to the path of motion of R (which is horizontal) to represent the velocity of R (i.e.v_{ R }). The vectors dr and o_{1} r intersect at r.
By measurement, we find that velocity of the ram R,
v_{ R }=\text { vector } o_{1} r=1.44 m / s
2. Angular velocity of link O_{2} D
By measurement from velocity diagram, we find that velocity of D with respect to O _{2} or velocity of D,
v_{ DO 2}=v_{ D }=\text { vector } o_{2} d=1.32 m / s
We know that length of link O_{2} D = 1300 mm = 1.3 m. Therefore angular velocity of the link O_{2} D ,
\omega_{ DO _{2}}=\frac{v_{ DO 2}}{O_{2} D}=\frac{1.32}{1.3}=1.015 rad / s \text { (Anticlockwise about } \left.O_{2}\right)