In my physical chemistry book, it says:
In the study of molecular speeds, we must consider a range of speeds. If we don’t, the probability would be zero. This probability is proportional to the range $\mathrm du_x$. Maxwell, based on probability theory, deduced that it is also proportional to $\mathrm e^{-\frac\beta3}$ or $\mathrm e^{-\frac{\beta u^2}2}$, where $\beta$ is a constant. Therefore, we can express the differential probability $\mathrm dP_x$ that a molecule has a speed component along the $x$-axis between $u_x$ and $u_x +\mathrm du_x$ as $\mathrm dP_x = B e^{-mu_x^2\beta/2}\mathrm du_x$
My question is trying to understand what $\mathrm dP_x$ is. I always like to think of the original functions, if we were to divide both sides by $\mathrm du_x$ and integrate, does that mean we are getting a cumulative distribution function or probability density function or what? if $\mathrm dP_x$ is a small change in $P_x$, what is $P_x$?