311 C H12

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    311 C H12 - Presentation Transcript

      • IV.) Torsion on Circular Shafts
      • A.) Torque (T)
    1.  
      • B.) Torsional Shearing Stress (  v )
      • -Under Pure Torsional Shear, experiments have shown that for circular shafts of constant cross-section:
      • 1.) Plane section remains plane.
      • 2.) A straight line radius remains a straight line.
    2. T A B B’ O FIXED END
    3. T Plane Sections Straight Line Radius  L T
    4.  
    5.  
      • From Hooke’s Law, Stress is directly proportional to strain.
      T  v
      • Consider a very small square area of a circular cross-section.
      T  v r c Area=a
      • The Stress on area “a” is:
      •  =   V (r)
      • c
      • The Force on area “a” is:
      • F =  a  =   V r(a)
      • c
      • The moment produced by this force on area “a” is:
      • M = F(r)  =   V ra(r) =  V ar 2
      • c c
          • The total moment produced by the forces on all the small areas gives you the torqe resistance of the cross-section:
      • T =  M =   V ar 2 =  V (  ar 2 ) c c
      • From Statics, recall that the Polar Moment of Inertia (J) is defined as:
      • J =  ar 2
      • Therefore: T =  V J
      • c
      • Therefore the torque resistance of a section of a given diameter at a maximum stress level  V is:
      • T =  V J
      • c
      • Or, the stress produced by a torque T, on a section of a given diameter is:
      •  V = Tc
      • J
      • B.) Angle of twist, 
      • Shearing strain is defined in Ch.9
      • in terms of the shear deformation,  v as:
      •  v =  v /L
       L T
      • In the sketch shown, the shear deformation is the distance BB’, therefore:
      •  v =BB’/L
      T O B B’  c
      • From geometry, we know that the arc length BB’ = c  therefore:
      • 
      •  v = c 
      • L
       c T O B B’
      • Since Hooke’s Law states:
      • G=  v /  v
      • we can substitute in the
      • above expression for  v :
      • G=  v __ =  v L
      • c  /L c 
       c T O B B’
      • Solving for  :
      •  =  v L (One formula for 
      • G c
      •  V = Tc
      • J
      •  =  v L = ( T c ) L = TL ( 2 nd formula for 
      • G c (J)G c JG
    6. Summary of Torsion Formulas
      •  = Angle of twist (radians)
      •  V = Shear Stress (psi)
      • L = Length (inches)
      • T = Torque (in-lb)
      • G = Modulus of Rigidity (psi)
      • c = Outside radius of shaft (inches)
      • J = Polar Moment of Inertia (in 4 )
       =  v L = TL G c JG  V = Tc J
      • A solid steel circular shaft is 4.5 feet long and has a diameter of 5 inches. If the shaft is fixed at one end a torque of 15,000 ft-lb is applied at the free end, find:
      • 1.) the maximum shear stress in the shaft and show where it occurs (on the sketch provided).
      • 2.) the shear stress at the center of the cross-section (point O).
      • 3.) the angle of twist at the free end.

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