What is the nature of strain as a physical quantity?
It is dimensionless.
Strain is the measure of deformation of a body relative to its original size. For direct (normal) strain it is defined as the change in length divided by the original length:
ε = δL / L
Here δL (the change in length) and L (the original length) are both lengths, carrying the same unit (for example mm or m). When one length is divided by another, the units cancel completely, so strain comes out as a pure number. This makes strain a dimensionless quantity — its dimensional formula is M⁰L⁰T⁰. It is sometimes written with helper labels such as mm/mm or m/m, or expressed as a percentage or in microstrain (με), but these are only conveniences; fundamentally the ratio equals a unitless number.
Therefore the correct description is that strain is dimensionless.
Hence strain, being a length-to-length ratio, is dimensionless.
A cylindrical steel rod with a diameter of 20 mm is subjected to a tensile load of 40 kN. The material has a yield strength of 450 MPa. Assuming the deformation remains within the elastic limit, calculate the factor of safety based on the ultimate tensile strength and the yield strength. If the modulus of elasticity of the steel is 200 GPa, determine the elongation of the rod over a length of 500 mm under this load. Which of the following options correctly represents the factor of safety based on yield strength and the elongation?
When a mild steel bar is loaded in tension within the elastic limit, the relation between stress and strain is:
A prismatic bar has
The materials which exhibit the same elastic properties in all direction are called
If a material has an infinitely large modulus of elasticity ($E$), it is considered to be
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.