Let S be the set of all the natural numbers, for which the line
\(\frac{x}{a}+\frac{y}{b}=2 \)
is a tangent to the curve
\((\frac{x}{a})^n+(\frac{y}{b})^n=2 \)
at the point (a, b), ab ≠ 0. Then :
\(S=\left\{2k:k∈N\right\}\)
\(S=N\)
The correct answer is (D) : S=N
\((\frac{x}{a})^n+(\frac{y}{b})^n=2 \)
\(⇒\frac{n}{a}(\frac{x}{a})^{n-1} +\frac{n}{b}(\frac{y}{b})^{n-1}\frac{dy}{dx} =0\)
\(⇒\frac{dy}{dx}=-\frac{b}{a}(\frac{bx}{ay})^{n-1}\)
\(\frac{dy}{dx_{(a,b)}}=-\frac{b}{a}\)
So line always touches the given curve.
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 :

m×n = -1
