If a material has an infinitely large modulus of elasticity ($E$), it is considered to be
perfectly rigid
The modulus of elasticity, often denoted by $E$, is a fundamental material property that measures its stiffness. It describes the relationship between stress and strain in the elastic region of deformation.
The relationship is defined by Hooke's Law for uniaxial stress:
$ \sigma = E \epsilon $
where:
The question states that a material has an infinitely large modulus of elasticity ($E \to \infty$). We can rearrange Hooke's Law to solve for strain:
$ \epsilon = \frac{\sigma}{E} $
If $ E $ approaches infinity ($ E \to \infty $) while the stress $ \sigma $ remains finite, the strain $ \epsilon $ must approach zero:
$ \epsilon \to \frac{\sigma}{\infty} \to 0 $
A strain of zero means there is no deformation or change in shape, regardless of the applied stress.
Based on the implication of zero strain:
Therefore, a material with an infinitely large modulus of elasticity ($E \to \infty$) is considered perfectly rigid because it experiences zero strain under any applied stress.
A prismatic bar has
The materials which exhibit the same elastic properties in all direction are called
A prismatic bar of rectangular cross- section is suspended freely from the ceiling of a roof. If all dimensions of the bar are doubled, then the total elongation produced by its own weight will increase by:
Stress developed due to application of a load suddenly is ______ times that due to same load Being applied gradually.
A rod of uniform cross-section A and length L is deformed by δ, when subjected to a normal force P. The Young’s modulus E of the material is