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**Hint**When a body is deformed by an external force, the internal restoring forces will oppose this force and restore the original shape of the object. This restoring force developed per unit area is called stress. The ratio of change in dimension to the original dimension is called strain.

**Complete Step by step solution**

According to Hooke’s law within the elastic limit, stress is proportional to strain

Stress $ \propto $strain

$ \Rightarrow \dfrac{{stress}}{{strain}} = const$

This constant is called the modulus of elasticity.

Stress can be defined as the force per unit area, i.e.

Stress = $\dfrac{F}{a}$

We know that force, $F = ma$

The dimensional formula for force is $F = m \times a = \left[ {ML{T^{ - 2}}} \right]$

The area is given by length $ \times $breadth

The dimensional formula for the area can be written as, $a = l \times b = \left[ {{M^0}{L^2}{T^0}} \right]$

The dimensional formula for stress can be written as,

Stress $ = \dfrac{{\left[ {ML{T^{ - 2}}} \right]}}{{\left[ {{M^0}{L^2}{T^0}} \right]}}$

The dimensional formula for linear stress can be written as,

Stress $ = \left[ {M{L^{ - 1}}{T^{ - 2}}} \right]$

The strain is a dimensionless quantity.

Therefore, the dimensional formula for modulus of elasticity can be written as,

Modulus of elasticity $ = \dfrac{{\left[ {M{L^{ - 1}}{T^{ - 2}}} \right]}}{{\left[ {{M^0}{L^0}{T^0}} \right]}} = \left[ {M{L^{ - 1}}{T^{ - 2}}} \right]$

**The answer is: Option (A): $\left[ {M{L^{ - 1}}{T^{ - 2}}} \right]$**

**Additional information**

An equation connecting the physical quantity with its dimensional formula is called the dimensional equation of that physical quantity. The dimensions of the same fundamental quantity must be the same on either side of a dimensional equation.

**Note**

All physical quantities can be expressed as a combination of seven fundamental or base quantities. The dimensional formula of a given physical quantity is an expression showing the dimensions of the fundamental quantities. Dimensions of a physical quantity are the powers to which the base quantities are to be raised to represent that quantity.

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