\(\frac{2^n}{m+1}-\frac{n}{m+1}(m+1,n-1)\)
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 center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity): 
Let $ a_0, a_1, ..., a_{23} $ be real numbers such that $$ \left(1 + \frac{2}{5}x \right)^{23} = \sum_{i=0}^{23} a_i x^i $$ for every real number $ x $. Let $ a_r $ be the largest among the numbers $ a_j $ for $ 0 \leq j \leq 23 $. Then the value of $ r $ 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:
