Question : A quick return mechanism of the crank and slotted lever type...

A quick return mechanism of the crank and slotted lever type shaping machine is shown in Fig. 7.17.
The dimensions of the various links are as follows :
O_{1} O_{2}=800 mm ; O _{1} B =300 mm;
O_{2} D=1300 mm ; D R=400 mm.
The crank O_{1} B makes an angle of 45^{\circ} with the vertical and rotates at 40 r.p.m. in the counter clockwise direction. Find : 1. velocity of the ram R, or the velocity of the cutting tool, and 2. angular velocity of link O_{2} D.

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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)

 

7.7.1
7.7.2