1. The given integral is:
\( I(R) = \int_{0}^{R} e^{-R \sin x} \, dx. \)
2. The term \( e^{-R \sin x} \) involves an exponential function with an oscillating argument \( \sin x \). The oscillatory nature of \( \sin x \) leads to variable behavior of the integrand \( e^{-R \sin x} \), which complicates direct evaluation.
3. To evaluate this integral analytically:
4. The expression \( \frac{\pi}{2R}(1 - e^{-R}) \) comes from approximations often used for integrals with oscillatory terms, but it is not exact.
5. Since \( I(R) \) and \( \frac{\pi}{2R}(1 - e^{-R}) \) involve different behaviors depending on \( R \), they cannot be directly compared for all values of \( R > 0 \).
Let $ I_1 = \int_{\frac{1}{2}}^{1} 2x \cdot f(2x(1 - 2x)) \, dx $
and $ I_2 = \int_{-1}^{1} f(x(1 - x)) \, dx \; \text{then} \frac{I_2}{I_1} \text{ equals to:} $

A quantity \( X \) is given by: \[ X = \frac{\epsilon_0 L \Delta V}{\Delta t} \] where:
- \( \epsilon_0 \) is the permittivity of free space,
- \( L \) is the length,
- \( \Delta V \) is the potential difference,
- \( \Delta t \) is the time interval.
The dimension of \( X \) is the same as that of: