\(∫_0^ 1 \frac{ 1}{7^{[\frac{1}{z}}]}dx\), let \(\frac{1}{x}=t\)
\(\frac{−1}{x^2}dx=dt\)
=\(∫_∞ ^1 \frac{1}{−t^27[t]}dt=∫_1 ^∞ \frac{1}{t^27[t]}dt\)
=\(∫_1^ 2 \frac{1}{7t^2}dt+∫_2 ^3 \frac{1}{7^2t^2}dt+…\)
=\(\frac{1}{7}\bigg[−\frac{1}{t}\bigg]_1^ 2+\frac{1}{7 ^2}\bigg[\frac{−1}{t}\bigg]_2^ 3+\frac{1}{7 ^3}\bigg[\frac{−1}{t}\bigg]_2^ 3+…\)
=\(∑_{n=1} ^∞\frac{1}{7_n}\bigg(\frac{1}{n}−\frac{1}{n+1}\bigg)\)
=\(∑_{n=1} ^∞\frac{(\frac{1}{7})^n}{n}−7∑_{n=1} ^∞\frac{(\frac{1}{7})^{n+1}}{n+1}\)
=\(−log\bigg(1−\frac{1}{7}\bigg)+7log\bigg(1−\frac{1}{7}\bigg)+1\)
=\(1+6\log\frac{6}{7}\)
Let \( f : (0, \infty) \to \mathbb{R} \) be a twice differentiable function. If for some \( a \neq 0 \), } \[ \int_0^a f(x) \, dx = f(a), \quad f(1) = 1, \quad f(16) = \frac{1}{8}, \quad \text{then } 16 - f^{-1}\left( \frac{1}{16} \right) \text{ is equal to:}\]
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 :

The representation of the area of a region under a curve is called to be as integral. The actual value of an integral can be acquired (approximately) by drawing rectangles.
Also, F(x) is known to be a Newton-Leibnitz integral or antiderivative or primitive of a function f(x) on an interval I.
F'(x) = f(x)
For every value of x = I.
Integral calculus helps to resolve two major types of problems: