2 Continued on next page... As the machine pulls the specimen, it stretches – not a great deal, but enough to register on the strain gauge. If we gradually increase the pulling force, the amount of strain will also increase. A force of 20 kilonewtons (4500 lb.) will cause twice the strain produced by a force of 10 kilonewtons (2250 lb.). The steel is elastic. Until the elastic limit of the specimen has been reached, the amount of strain will be directly proportional to the amount of pull, and the specimen will always return to its original length if the pulling force is released. If we continue to apply pulling force at a gradually increasing rate, watching both the force and strain gauge hands closely, we reach a point where the strain gauge hand continues to move while the force gauge hand remains stationary, or even drops a bit. We have now reached the elastic limit of the steel. If at this point, the pulling force is released, the specimen will not return to its original length. It has undergone permanent deformation. The force required to produce a slight amount of permanent deformation, expressed as megapascals (MPa) or pounds per square inch (psi) of specimen cross-section, is termed yield point or yield strength. If, instead of releasing the pulling force when the yield point has been reached, we continue to increase that force, the test specimen will stretch at a more rapid rate until the pulling force reaches a maximum point. Then it will begin to ”neck down” or grow visibly narrower at some point; the force gauge hand will start to drop, while the hand on the strain gauge will continue to climb. Then the specimen will break, after ”necking down” substantially. The value established by the highest reading registered on the force gauge is termed the tensile strength or ultimate tensile strength of the steel. To be more specific: The ultimate tensile strength is the maximum force registered on Fig. 8-1. Tensile strength is expressed in terms of the directly-applied pull required to break apart.
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