torsion of circular shaft
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NRI INSTITUTE OF INFORMATION SCIENCE & TECHNOLOGY
BHOPAL (M.P)
COMPILED BY AMIT SINGH 9827740442 ([email protected]) Page 1
TORSION OF CIRCULAR SHAFT
When a circular shaft is subjected to torsion, shear stresses are set up in the
material of the shaft. To determine the magnitude of shear stress at any point onthe shaft, consider a shaft fixed at one end AA and free at the end BB as shown.
Let CD is any line on the outer surface of the shaft. Now let the shaft is subjected
to a torque T at the end BB as shown. As a result of this torque T, the shaft at the
end BB will rotate clockwise and every cross-section of the shaft will be subjected
to shear stresses. The point D will shift to D’ and hence line CD will be deflected to
CD’ and the line OD’ will be shifted to OD’.
R = Radius of the shaft.
L = Length of the shaft.
T = torque applied at the end BB.
τ = Shear stress induced at the surface of the
shaft due to torque T.
C = Modulus of rigidity of the material of the
shaft.
Also equal to shear strain.
And is also called angle of twist.
If is very small than
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NRI INSTITUTE OF INFORMATION SCIENCE & TECHNOLOGY
BHOPAL (M.P)
COMPILED BY AMIT SINGH 9827740442 ([email protected]) Page 2
So
Now in the next figure we find the arc
So now the
Now the modulus of rigidity C of the material of the shaft is given as
So we will get
Now for a given shaft subjected to a given torque T, the value of C, ϴ and L are
constant. Hence shear stress produced is proportional to the radius R.
If q is the shear stress induced at a radius r from the center of the shaft then
The above equation is called torsion equation.
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NRI INSTITUTE OF INFORMATION SCIENCE & TECHNOLOGY
BHOPAL (M.P)
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From the above equation it is clear that shear stress at a point in the shaft is
proportional to the distance of the point from the axis of the shaft. Hence the
shear stress is Maximum at the outer surface and shear stress is zero at the axis of
the shaft.
MAXIMUM TORQUE TRANSMITTED BY A CIRCULAR SOLID SHAFT
The maximum torque transmitted by a circular solid shaft, is obtained from the
maximum shear stress induced at the outer surface of the solid shaft. Consider a
shaft subjected to a torque T as shown
τ=Maximum shear stress induced at the outer surface
R=Radius of the shaft
q=Shear stress at a radius r from the center
Consider an elementary circular ring of thickness ‘dr’ at a distance r from the
center as shown
Then the area of the ring
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NRI INSTITUTE OF INFORMATION SCIENCE & TECHNOLOGY
BHOPAL (M.P)
COMPILED BY AMIT SINGH 9827740442 ([email protected]) Page 4
From the equation
Shear stress at the radius r
Turning force on the elementary circular ring=
= Shear stress acting on the ring Area of the ring
Now turning moment due to turning force on the elementary ring
The total turning moment (or total torque) is obtained by integrating the above
equation between 0 to R
∫
∫
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NRI INSTITUTE OF INFORMATION SCIENCE & TECHNOLOGY
BHOPAL (M.P)
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Torque transmitted by a hollow circular shaft
POWER TRANSMITTED BY THE SHAFTS
Once the expression for torque T for a solid or a hollow shaft is obtained, power
transmitted by the shafts can be determined.
Let
EXPRESSION FOR TORQUE IN TERM OF POLAR MOMENT OF INERTIA
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NRI INSTITUTE OF INFORMATION SCIENCE & TECHNOLOGY
BHOPAL (M.P)
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POINT TO REMEMBER
(i) When two shafts are connected in series each shaft transmits the same
torque; the angle of twist is the sum of the angles of twist of the two
shafts.
(ii) The shafts are said to be in parallel when the driving torque is applied at
the junction of the shafts and resisting torque is at the other ends of the
shafts. Here the angle of twist is same for each shaft, but the applied
torque is divided between the two.
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NRI INSTITUTE OF INFORMATION SCIENCE & TECHNOLOGY
BHOPAL (M.P)
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STRAIN ENERGY STORED IN A BODY DUE TO TORSION
Consider a solid shaft which is in torsion. Take an elementary ring of width ‘dr’ at
the radius r as shown.
Then shear stress due to torsion at a radius r from the center is given by
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Total strain energy stored in the shaft is obtained by integrating the above
equation between 0 to R.
∫
∫
∫
∫
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NRI INSTITUTE OF INFORMATION SCIENCE & TECHNOLOGY
BHOPAL (M.P)
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Total strain energy in the hollow shaft due to torsion
COMBINED BENDING & TORSION
When a shaft is transmitting torque or power, it is subjected to shear stresses. At
the same time the shaft is also subjected to bending moment due to gravity or
inertia loads. Due to bending moment, bending stresses are also set up in the
shaft. Hence each particle in a shaft is subjected to shear stress and bending
stress. For design purpose it is necessary to find the principal stresses, maximumshear stresses and strain energy. The principal stresses and maximum shear stress
when a shaft is subjected to bending and torsion, are obtained as
Consider any point on the cross-section of a shaft
Let
The torque T will produce shear stress at the point whereas the B.M. will produce
bending stress.
Let q = Shear stress at the point produced by the torque T and
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Maximum shear stress i.e. on the surface of the shaft
()
√
√
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√
For a hollow shaft
[ ] √
[
] √
[ ] √