I'm trying to understand some equations concerning isentropic nozzle flow, found here (under "flow analysis"):
https://en.wikipedia.org/wiki/Isentropic_nozzle_flow
We have this continuity equation:
$$\rho AV = (\rho+d\rho)(A+dA)(V+dV)$$
Then the next step is:
If only the first-order terms in a differential quantity are retained, continuity takes the form
$$ \frac{dV}{V}+\frac{dA}{A}+\frac{d\rho}{\rho} = 0 $$
I don't understand how this step was made. I understand the concept of approximating a function with Taylor series and neglecting higher order terms when working in small intervals, but I'm still having hard time following how the step was made. Could somebody help me and explain this in more detail? Thank you!
The way one usually goes about showing this is by imagining $dV$, $dA$, and $d\rho$ are themselves first-order small quantities. Then expand: $$\begin{align} \rho AV &= (\rho + d\rho)(A + dA)(V+dV) \\&= \rho A V + \rho A dV + \rho V dA + AVd\rho + \rho dA dV + A d\rho dV + V d\rho dA + d\rho dA dV \end{align}$$ Now the terms $dV dA$ or any other term with at least two first-order small quantities multiplied together is a second-order small quantity (or higher-order) and can be assumed to be zero if the first-order small quantity is small. So we have: $$ \rho AV = \rho A V + \rho A dV + \rho V dA + AVd\rho $$ Divide both sides by $\rho AV$: $$ 1 = 1 + \frac{dV}{V} + \frac{dA}{A} + \frac{d\rho}{\rho}$$ And finally subtract $1$ from both sides: $$ 0 = \frac{dV}{V} + \frac{dA}{A} + \frac{d\rho}{\rho}$$
This presentation is a bit informal, but it gets the point across.