\(\frac{2^n}{m+1}-\frac{n}{m+1}(m+1,n-1)\)
The correct option is:(A) \(\frac{2^n}{m+1}-\frac{n}{m+1}(m+1,n-1)\).
Here, I(m,n) =\(\int_0^1 t^m(1+t)n dt ,\) reduce into I(m + 1, n - 1)
[we apply integration by parts taking (1 + t)\(^n\) as first
and t\(^m\) as second function]
\(\therefore \, \, \, \, \, i(m,n)=\bigg[(1+t)^n.\frac{t^{m+1}}{m+1}\bigg]_0^1 \, -\int_0^1n(1+t)^{n-1}.\frac{t^{m+1}}{m+1}dt\)
\(\, \, \, \, \, \, \, \, =\frac{2^n}{m+1}-\frac{n}{m+1} \int_0^1 (1+t)^{(n-1)},t^{m+1}dt\)
\(\therefore \, \, I(m,n) =\frac{2^n}{m+1}-\frac{n}{m+1}.I(m+1,n-1)\)
The left and right compartments of a thermally isolated container of length $L$ are separated by a thermally conducting, movable piston of area $A$. The left and right compartments are filled with $\frac{3}{2}$ and 1 moles of an ideal gas, respectively. In the left compartment the piston is attached by a spring with spring constant $k$ and natural length $\frac{2L}{5}$. In thermodynamic equilibrium, the piston is at a distance $\frac{L}{2}$ from the left and right edges of the container as shown in the figure. Under the above conditions, if the pressure in the right compartment is $P = \frac{kL}{A} \alpha$, then the value of $\alpha$ is ____
Let $ S $ denote the locus of the point of intersection of the pair of lines $$ 4x - 3y = 12\alpha,\quad 4\alpha x + 3\alpha y = 12, $$ where $ \alpha $ varies over the set of non-zero real numbers. Let $ T $ be the tangent to $ S $ passing through the points $ (p, 0) $ and $ (0, q) $, $ q > 0 $, and parallel to the line $ 4x - \frac{3}{\sqrt{2}} y = 0 $.
Then the value of $ pq $ is
Integration by Parts is a mode of integrating 2 functions, when they multiplied with each other. For two functions ‘u’ and ‘v’, the formula is as follows:
∫u v dx = u∫v dx −∫u' (∫v dx) dx
The first function ‘u’ is used in the following order (ILATE):
The rule as a diagram: