To determine the extension in length of the wire, we apply the formula from Hooke's Law relating stress, strain, and Young’s modulus: \( \text{Strain} = \frac{\text{Stress}}{E} \), where \( \text{Stress} = \frac{\text{Force}}{\text{Area}} \) and \( E \) is Young’s Modulus.
Therefore, the wire will extend in length by 20 μm, fitting perfectly within the expected range.
Step 1: Relation between stress and strain Young’s modulus is given by:
\[ Y = \frac{\text{Stress}}{\text{Strain}} = \frac{\frac{F}{A}}{\frac{\Delta \ell}{\ell}}. \]
Rearranging for \( \Delta \ell \):
\[ \Delta \ell = \frac{F \ell}{A Y}. \]
Step 2: Substitute given values
Substitute into the formula:
\[ \Delta \ell = \frac{200 \cdot 2}{2 \cdot 10^{-4} \cdot 10^{11}}. \]
Step 3: Simplify the expression
\[ \Delta \ell = \frac{400}{2 \times 10^7} = 2 \times 10^{-5} \, \text{m}. \]
Convert to micrometers (\( \mu \text{m} \)):
\[ \Delta \ell = 20 \, \mu \text{m}. \]
Final Answer: 20 \( \mu \text{m} \).
Temperature of a body \( \theta \) is slightly more than the temperature of the surroundings \( \theta_0 \). Its rate of cooling \( R \) versus temperature \( \theta \) graph should be 
MX is a sparingly soluble salt that follows the given solubility equilibrium at 298 K.
MX(s) $\rightleftharpoons M^{+(aq) }+ X^{-}(aq)$; $K_{sp} = 10^{-10}$
If the standard reduction potential for $M^{+}(aq) + e^{-} \rightarrow M(s)$ is $(E^{\circ}_{M^{+}/M}) = 0.79$ V, then the value of the standard reduction potential for the metal/metal insoluble salt electrode $E^{\circ}_{X^{-}/MX(s)/M}$ is ____________ mV. (nearest integer)
[Given : $\frac{2.303 RT}{F} = 0.059$ V]
An infinitely long straight wire carrying current $I$ is bent in a planar shape as shown in the diagram. The radius of the circular part is $r$. The magnetic field at the centre $O$ of the circular loop is :
