We split the integral into two parts based on the definition of \(F(x)\):
\[ \int_0^2 xF(x)dx = \int_0^1 xe^{x^2}dx + \int_1^2 xe^x dx \]
Let:
Use the substitution \(u = x^2 \Rightarrow du = 2x dx\). The limits change as:
The integral becomes:
\[ I_1 = \frac{1}{2} \int_0^1 e^u du \]
Evaluate the integral of \(e^u\):
\[ I_1 = \frac{1}{2} \left[e^u\right]_0^1 = \frac{1}{2} \left(e^1 - e^0\right) = \frac{1}{2}(e - 1) \]
Since \(e^x\) is constant with respect to \(x\), the integral becomes:
\[ I_2 = e \int_1^2 x dx \]
Evaluate the integral of \(x\):
\[ \int_1^2 x dx = \frac{x^2}{2} \bigg|_1^2 = \frac{2^2}{2} - \frac{1^2}{2} = \frac{4}{2} - \frac{1}{2} = \frac{3}{2} \]
Thus:
\[ I_2 = e \cdot \frac{3}{2} = \frac{3}{2}e \]
Add \(I_1\) and \(I_2\) to find the total integral:
\[ \int_0^2 xF(x)dx = I_1 + I_2 = \frac{1}{2}(e - 1) + \frac{3}{2}e \]
Combine terms:
\[ \int_0^2 xF(x)dx = \frac{1}{2}e - \frac{1}{2} + \frac{3}{2}e = \frac{4}{2}e - \frac{1}{2} = 2e - \frac{1}{2} \]
\[ \int_0^2 xF(x)dx = 2e - \frac{1}{2} \]
The value \( 9 \int_{0}^{9} \left\lfloor \frac{10x}{x+1} \right\rfloor \, dx \), where \( \left\lfloor t \right\rfloor \) denotes the greatest integer less than or equal to \( t \), is ________.
If the value of the integral
\[ \int_{-\frac{\pi}{2}}^{\frac{\pi}{2}} \left( \frac{x^2 \cos x}{1 + \pi^x} + \frac{1 + \sin^2 x}{1 + e^{\sin^x 2023}} \right) dx = \frac{\pi}{4} (\pi + a) - 2, \]
then the value of \(a\) is:
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,