mA = 48 kg ; mC = 20 kg ; rA = 15 mm = 0.015 m ; rC = 12.5 mm = 0.0125 m ; mB = 56 kg; rB = 15 mm = 0.015 m ; N = 300 r.p.m. or 0) = 2 rt x 300/60 = 31.42 rad/s.
1. Relative angular position of the pulleys The position of the shaft and pulleys is shown in Fig.(a) Let mL and mM = Mass at the bearings Land M, and rL and rM = Radius of rotation of the masses at Land M respectively. Assuming the plane of bearing L as reference plane, the data may be tabulated as below:
Plane (1) |
Mass (m) kg (2) |
Radius (r) m (3) |
Cent force/ω2(m.r) kg-m(4) |
Distance from plane L(l)m(5) |
Couple/ω2(m.r.l) kg-m2(6) |
A
L(R.P)
B
M
C |
48
mL
56
mM
20 |
.015
rL
0.015
rM
0.0125 |
0.72
mL.rL
0.84
mM.rM
0.25 |
-0.45
0
0.9
1.8
2.25
0.72
mL.rM
0.25 |
-0.324
0
0.756
1.8 mMrM
0.5625 |
First of all, draw the force polygon to some suitable scale, as shown in Fig. (c), from the data given in Table (column 4). It is assumed that the mass of pulley B acts in a vertical direction. We know that for the static balance of the pulleys, the centre of gravity of the system must lie on the axis of rotation. Therefore a force polygon must be a closed figure. Now in Fig.(b), draw OA parallel to vector bc and OC' parallel to vector co. By measurement, we find that Angle between pulleys B and A
= 1610 Ans. Angle between pulleys A and C = 760 and Angle between pulleys C and B = 1230.
Fig (a) Position of shaft of pulleys
Fig (b) Angular position of pulleys.
2. Dynamic forces at the two bearings In order to find the dynamic forces (or reactions) at the two bearings Land M, let us first calculate the values of m L. r L and m M.rM as discussed below:
Fig (c) Force polygon
Fig (d) Couple polygon
Fig (e) Force polygon
1. Draw the couple polygon to some suitable scale, as shown in Fig. (dL from the data given in Table (column 6).
The closing side of the polygon (vector co) represents the balanced couple and is proportional to 1.8 m M.rM. By measurement, we find that 1.8 m M. rM = vector c0 = 0.97 kg-m2 or m M. rM = 0.54 kg-m
Dynamic force at the bearing M = mM.rM.co2 = 0.54 (31.42) = 533 N
2. Now draw the force polygon, as shown in Fig.(e), from the data given in Table (column 4) and taking
mM.rM = 0.54 kg-m. The closing side of the polygon (vector do) represents the balanced force and is proportional to m L.rL. By measurement, we find that mL.rL = 0.54 kg-m
Dynamic force at the bearing L = mL.rL.CO2 = 0.54 (31.42)2 = 533 N