The given integral is of the form of the Beta function: \[ I(m, n) = \int_0^1 x^{m-1} (1-x)^{n-1} \, dx = B(m, n) \] where \( B(m, n) \) is the Beta function. We are asked to find \( I(9, 14) + I(10, 13) \).
Step 1: Use the recurrence relation of the Beta function The Beta function has the following recurrence relation: \[ B(m, n) + B(m+1, n-1) = B(m+1, n) \] Substituting the values of \( m = 9 \) and \( n = 14 \) into this recurrence relation, we get: \[ I(9, 14) + I(10, 13) = I(9, 13) \] This is because the integral \( I(9, 14) \) corresponds to \( B(9, 14) \) and \( I(10, 13) \) corresponds to \( B(10, 13) \), and using the recurrence relation we get that their sum is equal to \( I(9, 13) \), which corresponds to \( B(9, 13) \). Thus, the sum of the two integrals is: \[ I(9, 14) + I(10, 13) = I(9, 13) \]
A substance 'X' (1.5 g) dissolved in 150 g of a solvent 'Y' (molar mass = 300 g mol$^{-1}$) led to an elevation of the boiling point by 0.5 K. The relative lowering in the vapour pressure of the solvent 'Y' is $____________ \(\times 10^{-2}\). (nearest integer)
[Given : $K_{b}$ of the solvent = 5.0 K kg mol$^{-1}$]
Assume the solution to be dilute and no association or dissociation of X takes place in solution.
Inductance of a coil with \(10^4\) turns is \(10\,\text{mH}\) and it is connected to a DC source of \(10\,\text{V}\) with internal resistance \(10\,\Omega\). The energy density in the inductor when the current reaches \( \left(\frac{1}{e}\right) \) of its maximum value is \[ \alpha \pi \times \frac{1}{e^2}\ \text{J m}^{-3}. \] The value of \( \alpha \) is _________.
\[ (\mu_0 = 4\pi \times 10^{-7}\ \text{TmA}^{-1}) \]