I'm reading Calculus made easy to learn the notation (I know derivatives with the limit/prime style) and also some integral calculus which I haven't seen at school yet. You can check it here: https://www.gutenberg.org/files/33283/33283-pdf.pdf
$\color{red}{\texttt{page 32}}$
(9) The frequency n of vibration of a string of diameter D, length L and specific gravity σ, stretched with a force T, is given by
$$n = \frac{1}{DL} * \left( \frac{gT }{ πσ} \right)^{1/2}$$
Find the rate of change of the frequency when D, L, σ and T are varied singly
The answers are on $\color{red}{\texttt{page 252}}$. I know you have to treat everything as a constant except for what you are differentiating at the moment. For dn/dD you only work with D and every other letter is constant, for example.
My answers for dn/dD and dn/dL match the ones in the book... however, when I have to 'differentiate singly' stuff inside the square root I just can't get the algebra right (dn/dT and dn/dσ).
I post the derivative w.r.t T. You can first seperate the variable T from the others:
$n=\frac{1}{DL}\cdot \sqrt{\frac{g}{\pi \sigma}}\cdot \sqrt{T}$
Then you write $\sqrt T$ as $T^{1/2}$
$n=\underbrace{\frac{1}{DL}\cdot \sqrt{\frac{g}{\pi \sigma}}}_{\large{\begin{matrix} \texttt{constant in case of} \\ \texttt{ differentiation w.r.t. T} \end{matrix}}}\cdot T^{1/2}$
Therefore you need the derivative of $T^{1/2}$
$\frac{dn}{dT}=\frac{1}{DL}\cdot \sqrt{\frac{g}{\pi \sigma}}\cdot \frac{1}{2}\cdot T^{1/2-1}=\frac{1}{DL}\cdot \sqrt{\frac{g}{\pi \sigma}}\cdot \frac{1}{2}\cdot T^{-1/2}$
And $T^{-1/2}=\frac{1}{\sqrt{T}}=\sqrt{\frac{1}{T}}$
Now you can put all the terms under the radical together.
$\frac{dn}{dT}=\frac{1}{DL}\cdot \sqrt{\frac{g}{T\pi \sigma}}\cdot \frac{1}{2}=\frac{dn}{dT}=\frac{1}{2DL}\cdot \sqrt{\frac{g}{T\pi \sigma}}$
You can try the other derivative for yourself.