5.4 Two- and Three-Force           Members Simplify some equilibrium problems by recognizing embers that are subjected top...
5.4 Two- and Three-Force             MembersTwo-Force MembersExample  Forces at A and B are summed to  obtain their respec...
5.4 Two- and Three-Force          MembersTwo-Force Members Hence, only the force magnitude must be determined or stated Ot...
5.4 Two- and Three-Force                MembersThree-Force Members If a member is subjected to only three forces, it is ne...
5.4 Two- and Three-Force           MembersThree-Force Members To satisfy moment equilibrium about O, the third force must ...
5.4 Two- and Three-Force       Members          Bucket link AB on the back          hoe is a typical example of a         ...
5.4 Two- and Three-Force       Members        The boom ABD is subjected to the        weight of the suspended motor at D, ...
5.4 Two- and Three-Force               MembersExample 5.13The lever ABC is pin-supportedat A and connected to a shortlink ...
5.4 Two- and Three-Force            MembersSolutionFBD  Short link BD is a two-force  member, so the resultant  forces at ...
5.4 Two- and Three-Force            MembersSolutionFBD  For moment equilibrium, three  non-parallel forces acting on it  m...
5.4 Two- and Three-Force            MembersSolutionEquations of  Equilibrium           0 .7                 θ = tan −1 ...
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6161103 5.4 two and three-force members

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6161103 5.4 two and three-force members

  1. 1. 5.4 Two- and Three-Force Members Simplify some equilibrium problems by recognizing embers that are subjected top only 2 or 3 forcesTwo-Force Members When a member is subject to no couple moments and forces are applied at only two points on a member, the member is called a two-force member
  2. 2. 5.4 Two- and Three-Force MembersTwo-Force MembersExample Forces at A and B are summed to obtain their respective resultants FA and FB These two forces will maintain translational and force equilibrium provided FA is of equal magnitude and opposite direction to FB Line of action of both forces is known and passes through A and B
  3. 3. 5.4 Two- and Three-Force MembersTwo-Force Members Hence, only the force magnitude must be determined or stated Other examples of the two- force members held in equilibrium are shown in the figures to the right
  4. 4. 5.4 Two- and Three-Force MembersThree-Force Members If a member is subjected to only three forces, it is necessary that the forces be either concurrent or parallel for the member to be in equilibrium To show the concurrency requirement, consider a body with any two of the three forces acting on it, to have line of actions that intersect at point O
  5. 5. 5.4 Two- and Three-Force MembersThree-Force Members To satisfy moment equilibrium about O, the third force must also pass through O, which then makes the force concurrent If two of the three forces parallel, the point of currency O, is considered at “infinity” Third force must parallel to the other two forces to insect at this “point”
  6. 6. 5.4 Two- and Three-Force Members Bucket link AB on the back hoe is a typical example of a two-force member since it is pin connected at its end provided its weight is neglected, no other force acts on this member The hydraulic cylinder is pin connected at its ends, being a two-force member
  7. 7. 5.4 Two- and Three-Force Members The boom ABD is subjected to the weight of the suspended motor at D, the forces of the hydraulic cylinder at B, and the force of the pin at A. If the boom’s weight is neglected, it is a three-force member The dump bed of the truck operates by extending the hydraulic cylinder AB. If the weight of AB is neglected, it is a two-force member since it is pin-connected at its end points
  8. 8. 5.4 Two- and Three-Force MembersExample 5.13The lever ABC is pin-supportedat A and connected to a shortlink BD. If the weight of themembers are negligible,determine the force of the pinon the lever at A.
  9. 9. 5.4 Two- and Three-Force MembersSolutionFBD Short link BD is a two-force member, so the resultant forces at pins D and B must be equal, opposite and collinear Magnitude of the force is unknown but line of action known as it passes through B and D Lever ABC is a three-force member
  10. 10. 5.4 Two- and Three-Force MembersSolutionFBD For moment equilibrium, three non-parallel forces acting on it must be concurrent at O Force F on the lever at B is equal but opposite to the force F acting at B on the link Distance CO must be 0.5m since lines of action of F and the 400N force are known
  11. 11. 5.4 Two- and Three-Force MembersSolutionEquations of Equilibrium  0 .7  θ = tan −1   = 60.3 o  0.4  + → ∑ Fx = 0; FA cos 60.3o − F cos 45o + 400 N = 0 + ↑ ∑ Fy = 0; FA sin 60.3o − F sin 45o = 0Solving, FA = 1.07kN F = 1.32kN

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