141137 If $S$ is stress and $Y$ is Young's modulus of a material of wire, then energy stored in the wire per unit volume is:

141138 The breaking force for a wire of diameter $D$ of a material if $F$. The breaking force for a wire of the same material of radius $D$ is

141139 If in a wire of Young's modulus $Y$, longitudinal strain $X$ is produced then the potential energy stored in its unit volume will be:

141145 A rod elongates by $l$ when a body of mass $M$ is suspended from it. The work done is

141137 If $S$ is stress and $Y$ is Young's modulus of a material of wire, then energy stored in the wire per unit volume is:

141138 The breaking force for a wire of diameter $D$ of a material if $F$. The breaking force for a wire of the same material of radius $D$ is

141139 If in a wire of Young's modulus $Y$, longitudinal strain $X$ is produced then the potential energy stored in its unit volume will be:

141145 A rod elongates by $l$ when a body of mass $M$ is suspended from it. The work done is

141137 If $S$ is stress and $Y$ is Young's modulus of a material of wire, then energy stored in the wire per unit volume is:

141138 The breaking force for a wire of diameter $D$ of a material if $F$. The breaking force for a wire of the same material of radius $D$ is

141139 If in a wire of Young's modulus $Y$, longitudinal strain $X$ is produced then the potential energy stored in its unit volume will be:

141145 A rod elongates by $l$ when a body of mass $M$ is suspended from it. The work done is

141137 If $S$ is stress and $Y$ is Young's modulus of a material of wire, then energy stored in the wire per unit volume is:

141138 The breaking force for a wire of diameter $D$ of a material if $F$. The breaking force for a wire of the same material of radius $D$ is

141139 If in a wire of Young's modulus $Y$, longitudinal strain $X$ is produced then the potential energy stored in its unit volume will be:

141145 A rod elongates by $l$ when a body of mass $M$ is suspended from it. The work done is