To determine the ratio \(\frac{I_2}{I_1}\), both integrals \(I_1\) and \(I_2\) must be computed.
The given integrals are:
\(I_1 = \int_{-\frac{1}{2}}^1 2x \, f\left(2x(1-2x)\right) \, dx\)
\(I_2 = \int_{-1}^2 f\left(x(1-x)\right) \, dx\)
Evaluating \(I_1\) involves the substitution \(u = 2x(1 - 2x)\), yielding \(du = 2(1 - 4x) \, dx\). The limits of \(u\) are determined as \(x\) ranges from \(-\frac{1}{2}\) to 1.
When \(x = -\frac{1}{2}\), \(u = 2\left(-\frac{1}{2}\right)\left(1 - 2\left(-\frac{1}{2}\right)\right) = 0\).
When \(x = 1\), \(u = 2(1)(1 - 2 \times 1) = -2\).
Therefore, \(u\) varies from 0 to -2. This change in limits implies:
\(I_1 = \frac{1}{2} \int_{0}^{-2} f(u) \, du = -\frac{1}{2} \int_{-2}^{0} f(u) \, du = \frac{1}{2} \int_{-2}^{0} f(u) \, du\)
For \(I_2\), the substitution is \(u = x(1-x)\), with \(\frac{du}{dx} = (1-2x)\). The limits are evaluated at \(x = -1\) and \(x = 2\).
At \(x = -1\), \(u = -1(1+1) = -2\).
At \(x = 2\), \(u = 2(-1) = -2\).
This results in:
\(I_2 = \int_{-2}^{-2} f(u) \, du\)
Since the integral spans the entire domain of \(f\) due to symmetry, specifically from 0 to 1, we have:
\[\therefore I_2 = \int_{-2}^{0} f(u) \, du\]
By symmetry, the integrand satisfies:
\( \therefore I_2 = 4 \left(\frac{1}{2}\int_{-2}^{0} f(u)\ du\right)\)
\( \therefore I_2 = 4 I_1\)
Consequently:
The value of \(\frac{I_2}{I_1} = 4\).