\( \frac{1 + 5\sqrt{2}}{3} \)
\( \frac{5 + 4\sqrt{2}}{3} \)
\( \frac{5 + 4\sqrt{2}}{3} \)
\( \frac{4 + 5\sqrt{2}}{3} \)
We are given the function \( f(x) = \max \{ x^2, 1 + [x] \} \). Let's first break the integral into two parts based on the function's definition.
Step 1: Break the interval of integration.
We need to consider the behavior of the function in different intervals. The greatest integer function \( [x] \) takes integer values, and we evaluate the function \( f(x) \) on the interval from \( 0 \) to \( \sqrt{2} \).
- For \( 0 \leq x < 1 \), \( [x] = 0 \), so \( f(x) = \max \{ x^2, 1 \} \).
- For \( 1 \leq x < \sqrt{2} \), \( [x] = 1 \), so \( f(x) = \max \{ x^2, 2 \} \).
Step 2: Evaluate the integral.
Now, we can evaluate the integral over two separate intervals.
1. For the interval \( [0, 1] \), we have \( f(x) = 1 \), since \( x^2 \leq 1 \) for \( x \in [0, 1] \). Thus, the integral is: \[ \int_0^1 1 \, dx = 1. \] 2. For the interval \( [1, \sqrt{2}] \), we have \( f(x) = x^2 \), since \( x^2 \geq 2 \) for \( x \in [1, \sqrt{2}] \). Thus, the integral is: \[ \int_1^{\sqrt{2}} x^2 \, dx = \left[ \frac{x^3}{3} \right]_1^{\sqrt{2}} = \frac{(\sqrt{2})^3}{3} - \frac{1^3}{3} = \frac{2\sqrt{2}}{3} - \frac{1}{3}. \]
Step 3: Combine the results.
Now, combine the results of the two integrals: \[ \int_0^{\sqrt{2}} f(x) \, dx = 1 + \frac{2\sqrt{2}}{3} - \frac{1}{3} = 1 + \frac{2\sqrt{2} - 1}{3}. \] Simplifying further: \[ 1 + \frac{2\sqrt{2} - 1}{3} = \frac{3}{3} + \frac{2\sqrt{2} - 1}{3} = \frac{3 + 2\sqrt{2} - 1}{3} = \frac{5 + 4\sqrt{2}}{3}. \] Thus, the value of the integral is \( \frac{5 + 4\sqrt{2}}{3} \), and the correct answer is option (2).
What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,