\[ \lim_{x \to 0} 2 \cdot \frac{\left( 1 - \frac{x^2}{2!} \right) \left( 1 - \frac{4x^2}{2!} \right) \left( 1 - \frac{9x^2}{2!} \right) \cdots \left( 1 - \frac{100x^2}{2!} \right)}{x^2} \]
By expansion:
\[ \lim_{x \to 0} 2 \cdot \frac{\left[ 1 - \frac{x^2}{2} \right] \left[ 1 - \frac{2x^2}{2} \right] \left[ 1 - \frac{3x^2}{2} \right] \cdots \left[ 1 - \frac{10x^2}{2} \right]}{x^2}. \]
Simplify the product:
\[ \lim_{x \to 0} 2 \cdot \frac{1 - \left[ \frac{x^2}{2} + \frac{2x^2}{2} + \frac{3x^2}{2} + \cdots + \frac{10x^2}{2} \right]}{x^2}. \]
The \(x^2\) terms cancel:
\[ 2 \cdot \left( \frac{1}{2} + \frac{2}{2} + \frac{3}{2} + \cdots + \frac{10}{2} \right). \]
Simplify the summation:
\[ 2 \cdot \frac{1 + 2 + 3 + \cdots + 10}{2}. \]
The sum of the first 10 natural numbers is:
\[ \frac{10 \cdot 11}{2} = 55. \]
Final Answer: 55.
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 :
