I am following a Physics textbook where the author has written the following using the chain rule:
$\begin{align} \frac{\partial f(y+\alpha \eta, y'+\alpha\eta', x)}{{\partial\alpha}} &=\eta\frac{\partial f}{\partial y}+\eta '\frac{\partial f}{\partial y'} \end{align}$
Here's how I have gone about it:
$ \begin{align} \frac{\partial f(y+\alpha \eta, y'+\alpha\eta', x)}{{\partial\alpha}} &= \frac{\partial f(y+\alpha \eta, y'+\alpha\eta', x)}{{\partial (y+\alpha \eta)}}\frac{\partial (y+\alpha \eta)}{\partial \alpha} \\& + \frac{\partial f(y+\alpha \eta, y'+\alpha\eta', x)}{{\partial (y'+\alpha \eta')}}\frac{\partial (y'+\alpha \eta')}{\partial \alpha} \\&+ \frac{\partial f(y+\alpha \eta, y'+\alpha\eta', x)}{{\partial x}}\frac{\partial x}{\partial \alpha} \\&= \eta\frac{\partial f}{\partial (y+\alpha \eta)}+\eta '\frac{\partial f}{\partial (y'+\alpha \eta')} + 0 \end{align} $
But how did $\partial (y+\alpha \eta)$ in the denominator become $\partial y$? Likewise for the other denominator $\partial (y'+\alpha \eta')$?
Thanks
Edit:
$\begin{align} \eta' &= \frac{d\eta}{ dx}\\y & = y(x)\end{align} $
Also, $\alpha$ is an independent parameter
Using the chain rule we note that $\frac{\partial}{\partial \alpha} = \frac{\partial y}{\partial \alpha} \frac{\partial}{\partial y} + \frac{\partial y'}{\partial \alpha} \frac{\partial}{\partial y'} = \eta \partial_y + \eta' \partial_{y'}$ \begin{align} \frac{\partial f}{{\partial\alpha}} &=\eta\frac{\partial f}{\partial y}+\eta '\frac{\partial f}{\partial y'} \\ \end{align}