Rotating Bodies - Stress
Stress in a Rotating Disc
Stress in a rotating disc can be calculated as
σz = ω2 r2 ρ / 3
= v2 ρ / 3
= ( 2 π n / 60)2r2ρ / 3 (1)
where
σz = stress (Pa, N/m2)
ω = angular velocity (rad/s)
r = radius of disc (m)
ρ = density (kg/m3)
π = 3.14...
n= revolutions per minute (rpm)
Stress in a Rotating Ring
Stress in a rotating ring can be calculated as
σz = ω2ρ (r12+ r1 r2+ r2 2) / 3 (2)
where
r1 = outer radius of ring (m)
r2= inner radius of ring (m)
For a thin ring the equation can be simplified to
σz = ω2 ρ r 2 (3)
where
r = mean radius of ring (m)
Design Stress for materials used in Flywheels
Material | Density (kg/m3) | Typical Design Stress (MPa) |
---|---|---|
Aluminum alloy | 2700 | |
Birch plywood | 700 | 30 |
Composite carbon fiber - 40% epoxy | 1550 | 750 |
E-glass fiber - 40% epoxy | 1900 | 250 |
Kevlar fiber - 40% epoxy | 1400 | 1000 |
Maraging steel | 8000 | 900 |
Titanium Alloy | 4500 | 650 |
"Super paper" | 1100 | |
S-glass fiber/epoxy | 1900 | 350 |
Related Topics
• Dynamics
Motion of bodies and the action of forces in producing or changing their motion - velocity and acceleration, forces and torque.
Related Documents
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The kinetic energy stored in flywheels - the moment of inertia.
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Stress in Thick-Walled Cylinders or Tubes
Radial and tangential stress in thick-walled cylinders or tubes with closed ends - with internal and external pressure.
Stress in Thin-Walled Cylinders or Tubes
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Stress, Strain and Young's Modulus
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