The quantities \( I_1 \) and \( I_2 \) are integrals involving the speed distribution function \( P(v) \), and they represent different moments of the speed distribution.
From the Maxwell-Boltzmann distribution, we know that the speed probability distribution \( P(v) \) is proportional to \( v^2 e^{-\frac{mv^2}{2kT}} \), where \( m \) is the mass of the molecules and \( T \) is the temperature.
### Step 1: Evaluate the relationship between \( I_1 \) and \( I_2 \).
- \( I_1 = \int_0^\infty P(v) v^3 \, dv \) is the moment that involves the \( v^3 \) term, which has a higher dependence on the velocity and is affected more by higher speeds.
- \( I_2 = \int_0^\infty P(v) v \, dv \) involves the \( v \) term and is less dependent on higher velocities.
In general, for any given distribution, the moment involving \( v^3 \) (which represents higher-order moments) will be smaller than the moment involving \( v \) since the integrand in \( I_1 \) decays faster than that in \( I_2 \) due to the higher powers of \( v \). This means that:
\[
I_1<I_2
\]
Thus, the correct relationship is \( I_1<I_2 \).