# for derivatives

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##### 1: 4.20 Derivatives and Differential Equations
###### §4.20 Derivatives and Differential Equations
4.20.9 $\frac{{\mathrm{d}}^{2}w}{{\mathrm{d}z}^{2}}+a^{2}w=0,$
4.20.10 $\left(\frac{\mathrm{d}w}{\mathrm{d}z}\right)^{2}+a^{2}w^{2}=1,$
##### 2: 4.34 Derivatives and Differential Equations
###### §4.34 Derivatives and Differential Equations
4.34.7 $\frac{{\mathrm{d}}^{2}w}{{\mathrm{d}z}^{2}}-a^{2}w=0,$
4.34.8 $\left(\frac{\mathrm{d}w}{\mathrm{d}z}\right)^{2}-a^{2}w^{2}=1,$
4.34.9 $\left(\frac{\mathrm{d}w}{\mathrm{d}z}\right)^{2}-a^{2}w^{2}=-1,$
4.34.10 $\frac{\mathrm{d}w}{\mathrm{d}z}+a^{2}w^{2}=1,$
##### 3: 4.7 Derivatives and Differential Equations
###### §4.7(i) Logarithms
4.7.5 $\frac{\mathrm{d}w}{\mathrm{d}z}=\frac{f^{\prime}(z)}{f(z)}$
##### 4: 22.13 Derivatives and Differential Equations
###### §22.13(i) Derivatives
Note that each derivative in Table 22.13.1 is a constant multiple of the product of the corresponding copolar functions. …
##### 5: 7.10 Derivatives
###### §7.10 Derivatives
7.10.1 $\frac{{\mathrm{d}}^{n+1}\operatorname{erf}z}{{\mathrm{d}z}^{n+1}}=(-1)^{n}% \frac{2}{\sqrt{\pi}}H_{n}\left(z\right)e^{-z^{2}},$ $n=0,1,2,\dots$.
$\frac{\mathrm{d}\mathrm{f}\left(z\right)}{\mathrm{d}z}=-\pi z\mathrm{g}\left(z% \right),$
$\frac{\mathrm{d}\mathrm{g}\left(z\right)}{\mathrm{d}z}=\pi z\mathrm{f}\left(z% \right)-1.$
##### 6: 1.5 Calculus of Two or More Variables
###### §1.5(i) Partial Derivatives
The function $f(x,y)$ is continuously differentiable if $f$, $\ifrac{\partial f}{\partial x}$, and $\ifrac{\partial f}{\partial y}$ are continuous, and twice-continuously differentiable if also $\ifrac{{\partial}^{2}f}{{\partial x}^{2}}$, $\ifrac{{\partial}^{2}f}{{\partial y}^{2}}$, $\,{\partial}^{2}f/\,\partial x\,\partial y$, and $\,{\partial}^{2}f/\,\partial y\,\partial x$ are continuous. …
###### §1.5(vi) Jacobians and Change of Variables
1.5.40 $\frac{\partial(f,g,h)}{\partial(x,y,z)}=\begin{vmatrix}\ifrac{\partial f}{% \partial x}&\ifrac{\partial f}{\partial y}&\ifrac{\partial f}{\partial z}\\ \ifrac{\partial g}{\partial x}&\ifrac{\partial g}{\partial y}&\ifrac{\partial g% }{\partial z}\\ \ifrac{\partial h}{\partial x}&\ifrac{\partial h}{\partial y}&\ifrac{\partial h% }{\partial z}\end{vmatrix},$
##### 7: 36.10 Differential Equations
###### §36.10(ii) Partial Derivatives with Respect to the $x_{n}$
36.10.7 $\frac{{\partial}^{2n}\Psi_{2}}{{\partial x}^{2n}}=i^{n}\frac{{\partial}^{n}% \Psi_{2}}{{\partial y}^{n}}.$
36.10.8 $\frac{{\partial}^{2n}\Psi_{3}}{{\partial x}^{2n}}=i^{n}\frac{{\partial}^{n}% \Psi_{3}}{{\partial y}^{n}},$
36.10.10 $\frac{{\partial}^{3n}\Psi_{3}}{{\partial y}^{3n}}=i^{n}\frac{{\partial}^{2n}% \Psi_{3}}{{\partial z}^{2n}}.$
##### 8: 19.18 Derivatives and Differential Equations
###### §19.18(i) Derivatives
Let $\partial_{j}=\ifrac{\partial}{\partial z_{j}}$, and $\mathbf{e}_{j}$ be an $n$-tuple with 1 in the $j$th place and 0’s elsewhere. …
19.18.14 $\frac{{\partial}^{2}w}{{\partial x}^{2}}=\frac{{\partial}^{2}w}{{\partial y}^{% 2}}+\frac{1}{y}\frac{\partial w}{\partial y}.$
19.18.15 $\frac{{\partial}^{2}W}{{\partial t}^{2}}=\frac{{\partial}^{2}W}{{\partial x}^{% 2}}+\frac{{\partial}^{2}W}{{\partial y}^{2}}.$
##### 9: 30.12 Generalized and Coulomb Spheroidal Functions
30.12.1 $\frac{\mathrm{d}}{\mathrm{d}z}\left((1-z^{2})\frac{\mathrm{d}w}{\mathrm{d}z}% \right)+{\left(\lambda+\alpha z+\gamma^{2}(1-z^{2})-\frac{\mu^{2}}{1-z^{2}}% \right)w}=0,$
30.12.2 $\frac{\mathrm{d}}{\mathrm{d}z}\left((1-z^{2})\frac{\mathrm{d}w}{\mathrm{d}z}% \right)+\left(\lambda+\gamma^{2}(1-z^{2})-\frac{\alpha(\alpha+1)}{z^{2}}-\frac% {\mu^{2}}{1-z^{2}}\right)w=0,$
##### 10: 14.29 Generalizations
14.29.1 $\left(1-z^{2}\right)\frac{{\mathrm{d}}^{2}w}{{\mathrm{d}z}^{2}}-2z\frac{% \mathrm{d}w}{\mathrm{d}z}+{\left(\nu(\nu+1)-\frac{\mu_{1}^{2}}{2(1-z)}-\frac{% \mu_{2}^{2}}{2(1+z)}\right)w}=0$