Shafts Torsion
The torsion of solid or hollow shafts - Polar Moment of Inertia of Area.
Shear Stress in the Shaft
When a shaft is subjected to a torque or twisting a shearing stress is produced in the shaft. The shear stress varies from zero in the axis to a maximum at the outside surface of the shaft.
The shear stress in a solid circular shaft in a given position can be expressed as:
τ = T r / J (1)
where
τ = shear stress (Pa, lbf /ft2(psf))
T = twisting moment (Nm, lbf ft)
r = distance from center to stressed surface in the given position (m, ft)
J = Polar Moment of Inertia of Area (m4 , ft4 )
Note
- the " Polar Moment of Inertia of an Area " is a measure of a shaft's ability to resist torsion. The " Polar Moment of Inertia" is defined with respect to an axis perpendicular to the area considered. It is analogous to the " Area Moment of Inertia " - which characterizes a beam's ability to resist bending - required to predict deflection and stress in a beam.
- 1 ft = 12 in
- 1 ft4 = 20736 in4
- 1 psf (lbf /ft2) = 1/144 psi (lbf /in2)
" Polar Moment of Inertia of an Area " is also called " Polar Moment of Inertia ", " Second Moment of Area ", " Area Moment of Inertia ", " Polar Moment of Area " or " Second Area Moment ".
Polar Moment of Inertia vs. Area Moment of Inertia
- " Polar Moment of Inertia " - a measure of a beam's ability to resist torsion - which is required to calculate the twist of a beam subjected to torque
- " Area Moment of Inertia " - a property of shape that is used to predict deflection, bending and stress in beams
Circular Shaft and Maximum Moment or Torque
Maximum moment in a circular shaft can be expressed as:
T max = τ max J / R (2)
where
T max = maximum twisting torque (Nm, lbf ft)
τ max = maximum shear stress (Pa, lbf /ft2)
R = radius of shaft (m, ft)
Combining (2) and (3) for a solid shaft
T max = (π / 16) τ max D3 (2b)
Combining (2) and (3b) for a hollow shaft
T max = (π / 16) τ max (D4 - d4 ) / D (2c)
Circular Shaft and Polar Moment of Inertia
Polar Moment of Inertia of a circular solid shaft can be expressed as
J = π R4 / 2
= π (D / 2)4 / 2
= π D4 / 32 (3)
where
D = shaft outside diameter (m, in)
Polar Moment of Inertia of a circular hollow shaft can be expressed as
J = π (D4 - d4) / 32 (3b)
where
d = shaft inside diameter (m, in)
Diameter of a Solid Shaft
Diameter of a solid shaft can calculated by the formula
D = 1.72 (T max / τ max )1/3 (4)
Torsional Deflection of Shaft
The angular deflection of a torsion shaft can be expressed as
α = L T / (JG) (5)
where
α = angular shaft deflection ( radians )
L = length of shaft (m, ft)
G = Shear Modulus of Rigidity - or Modulus of Rigidity (Pa, psf)
The angular deflection of a torsion solid shaft can be expressed as
α = 32 L T / (G π D4) (5a)
The angular deflection of a torsion hollow shaft can be expressed as
α = 32 L T / (G π (D4 - d4)) (5b)
The angle in degrees can be achieved by multiplying the angle θ in radians with 180 / π.
S olid shaft ( π replaced)
α degrees ≈ 584 L T / (G D4) (6a)
Hollow shaft (π replaced)
α degrees ≈ 584 L T / (G (D4 - d4) (6b)
Torsion Resisting Moments from Shafts of Various Cross Sections
Shaft Cross Section Area | Maximum Torsional Resisting Moment - T max - (Nm, lbf ft) | Nomenclature | |
---|---|---|---|
Solid Cylinder Shaft |
(π / 16) τ max (2 r)3 = (π / 16) τ max D3 |
||
Hollow Cylinder Shaft |
(π / 16) τ max ((2 R)4 - (2 r)4 ) / (2 R) = (π / 16) τ max (D4 - d4 ) / D |
||
Ellipse Shaft | (π / 16) τ max b2h | h = "height" of shaft b = "width" of shaft h > b |
|
Rectangle Shaft | (2 / 9) τ max b2h | h > b | |
Square Shaft | (2 / 9) τ max H3 | ||
Triangle Shaft | (1 / 20) τ max b3 | b = length of triangle side | |
Hexagon Shaft |
0.123τ max D3 0.189 τ max b 3 |
Example - Shear Stress and Angular Deflection in a Solid Cylinder
A moment of 1000 Nm is acting on a solid cylinder shaft with diameter 50 mm (0.05 m) and length 1 m . The shaft is made in steel with modulus of rigidity 79 GPa (79 109 Pa) .
Maximum shear stress can be calculated as
τ max = T r / J
= T (D / 2) / ( π D4 / 32)
= (1000 Nm) ((0.05 m) / 2) / ( π (0.05 m)4 / 32)
= 40764331 Pa
= 40.8 MPa
The angular deflection of the shaft can be calculated as
θ = L T / (J G)
= L T / ( ( π D4 / 32) G)
= (1 m) (1000 Nm) / ((π (0.05 m)4 / 32) (79 109 Pa))
= 0.021 ( radians)
= 1.2 o
Example - Shear Stress and Angular Deflection in a Hollow Cylinder
A moment of 1000 Nm is acting on a hollow cylinder shaft with outer diameter 50 mm (0.05 m) , inner diameter 30 mm (0.03 m) and length 1 m . The shaft is made in steel with modulus of rigidity 79 GPa (79 109 Pa) .
Maximum shear stress can be calculated as
τ max = T r / J
= T (D / 2) / (π (D4 - d4 ) / 32)
= (1000 Nm) ((0.05 m) / 2) / (π ((0.05 m)4 - (0.03 m)4 ) / 32)
= 46.8 MPa
The angular deflection of the shaft can be calculated as
θ = L T / (J G)
= L T / (( π D4 / 32) G)
= (1 m) (1000 Nm) / ( ( π ((0.05 m)4 - (0.03 m)4 ) / 32) (79 109 Pa))
= 0.023 radian)
= 1.4 o
Example - Required Shaft Diameter to Transmit Power
A 15 kW electric motor shall be used to transmit power through a connected solid shaft. The motor and the shaft rotates with 2000 rpm . The maximum allowable shear stress - τ max - in the shaft is 100 MPa .
The connection between power and torque can be expressed
P = 0.105 n rpm T (7)
where
P = power (W)
n rpm = speed of shaft (rpm)
Re-arranged and with values - the torque can be calculated
T = (15 103 W) / (0.105 (2000 rpm))
= 71 Nm
Minimum diameter of the shaft can be calculated with eq. 4
D = 1.72 ((71 Nm) / (100 106 Pa)) 1/3
= 0.0153 m
= 15.3 mm
Related Topics
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Mechanics
The relationships between forces, acceleration, displacement, vectors, motion, momentum, energy of objects and more. -
Statics
Forces acting on bodies at rest under equilibrium conditions - loads, forces and torque, beams and columns.
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