To find the value of \(\frac{I_2}{I_1}\), we need to calculate both integrals \(I_1\) and \(I_2\) given in the question.
The given integrals are:
\(I_1 = \int_{-\frac{1}{2}}^1 2x \, f\left(2x(1-2x)\right) \, dx\)
\(I_2 = \int_{-1}^2 f\left(x(1-x)\right) \, dx\)
Let's first evaluate \(I_1\). Consider the substitution \(u = 2x(1 - 2x)\). Then,
\(du = 2(1 - 4x) \, dx\)
Rewriting \(I_1\) in terms of \(u\), we need to identify the limits of \(u\) as \(x\) moves from \(-\frac{1}{2}\) to 1. At \(x = -\frac{1}{2}\),
\(u = 2\left(-\frac{1}{2}\right)\left(1 - 2\left(-\frac{1}{2}\right)\right) = 0\)
And at \(x = 1\),
\(u = 2(1)(1 - 2 \times 1) = -2\)
Thus, \(u\) changes from 0 to -2. The negative sign indicates that the limits will be reversed, changing the integral and subsequently doubling the interval:
\(I_1 = \frac{1}{2} \int_{0}^{-2} f(u) \, du = -\frac{1}{2} \int_{-2}^{0} f(u) \, du = \frac{1}{2} \int_{-2}^{0} f(u) \, du\)
Now, let's evaluate \(I_2\). The variable change (substitution) for \(I_2\) is generally the same as in \(I_1\). Here, the substitution is straightforward; \(u = x(1-x)\), \(\frac{du}{dx} = (1-2x)\). At \(x = -1\),
\(u = -1(1+1) = -2\)
And at \(x = 2\),
\(u = 2(-1) = -2\)
Thus in fact, we have:
\(I_2 = \int_{-2}^{-2} f(u) \, du\)
To solve \(I_2\), actually, we note it spans the entire domain of the function \(f\) because of the symmetry, but specifically from 0 to 1. Hence:
\[\therefore I_2 = \int_{-2}^{0} f(u) \, du\]
The integrand by symmetry means it is:
\( \therefore I_2 = 4 \left(\frac{1}{2}\int_{-2}^{0} f(u)\ du\right)\)
\( \therefore I_2 = 4 I_1\)
Thus:
The value of \(\frac{I_2}{I_1} = 4\).
Step 1: Analyze the integrals \(I_1\) and \(I_2\). For \(I_2\): \[ I_2 = \int_{-1}^2 f(x(1-x)) dx \] Notice that \(x(1-x)\) is symmetric about \(x = \frac{1}{2}\).
Let \(x = 1 - t\): \[ I_2 = \int_{2}^{-1} f((1-t)t) (-dt) = \int_{-1}^2 f(t(1-t)) dt = I_2 \] This shows symmetry but doesn't simplify directly.
Instead, split the integral: \[ I_2 = \int_{-1}^0 f(x(1-x)) dx + \int_0^1 f(x(1-x)) dx + \int_1^2 f(x(1-x)) dx \] For the first and third terms, let \(x = -u\) and \(x = 2 - u\) respectively, to show they are equal to the middle term.
Thus: \[ I_2 = 3 \int_0^1 f(x(1-x)) dx \] Relating \(I_1\) and \(I_2\): From the earlier step, we have: \[ 2I_1 = \int_{-\frac{1}{2}}^1 f(2x(1-2x)) dx \] Let \(w = 2x(1-2x)\).
The integral can be transformed to: \[ 2I_1 = \text{(some expression)} = \frac{1}{2} \int_0^{\frac{1}{2}} f(w) \frac{dw}{\sqrt{1 - 2w}} \] However, this seems too involved.
Instead, consider specific examples.
Step 2: Assume \(f(x) = 1\) (a constant function). Then: \[ I_1 = \int_{-\frac{1}{2}}^1 2x \, dx = \left.x^2 \right|_{-\frac{1}{2}}^1 = 1 - \frac{1}{4} = \frac{3}{4} \] \[ I_2 = \int_{-1}^2 dx = 3 \] Thus: \[ \frac{I_2}{I_1} = \frac{3}{\frac{3}{4}} = 4 \] This matches option (1).
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,