Kelvin functions

Plot of the Kelvin function ber(z) in the complex plane from -2-2i to 2+2i with colors created with Mathematica 13.1 function ComplexPlot3D

Plot of the Kelvin function ber(z) in the complex plane from -2-2i to 2+2i with colors created with Mathematica 13.1 function ComplexPlot3D

In applied mathematics, the Kelvin functions ber_ν(x) and bei_ν(x) are the real and imaginary parts, respectively, of

$J_{\nu }\left(x{e}^{\frac{3\pi i}{4}}\right),$

where x is real, and J_ν(z), is the ν^th order Bessel function of the first kind. Similarly, the functions ker_ν(x) and kei_ν(x) are the real and imaginary parts, respectively, of

$e^{-\nu \pi i/2}{K}_{\nu }\left(x{e}^{\frac{\pi i}{4}}\right),$

where K_ν(z) is the ν^th order modified Bessel function of the second kind.

These functions are named after William Thomson, 1st Baron Kelvin.

While the Kelvin functions are defined as the real and imaginary parts of Bessel functions with x taken to be real, the functions can be analytically continued for complex arguments xe^iφ, 0 ≤ φ < 2π. With the exception of ber_n(x) and bei_n(x) for integral n, the Kelvin functions have a branch point at x = 0.

Below, Γ(z) is the gamma function and ψ(z) is the digamma function.

ber(x)

File:Mplwp Kelvin-ber.svg

ber(x) for x between 0 and 20.

File:Mplwp Kelvin-ber-norm.svg

$\mathrm{b}\mathrm{e}\mathrm{r}(x)/e^{x/\sqrt{2}}$ for x between 0 and 50.

For integers n, ber_n(x) has the series expansion

${\mathrm{b}\mathrm{e}\mathrm{r}}_n(x)={\left(\frac{x}{2}\right)}^n\sum _{k\ge 0}\frac{\cos \left[(\frac{3n}{4}+\frac{k}{2})\pi \right]}{k!\Gamma (n+k+1)}{\left(\frac{x^2}{4}\right)}^k,$

where Γ(z) is the gamma function. The special case ber₀(x), commonly denoted as just ber(x), has the series expansion

$\mathrm{b}\mathrm{e}\mathrm{r}(x)=1+\sum _{k\ge 1}\frac{(-1{)}^k}{[(2k)!{]}^2}{\left(\frac{x}{2}\right)}^{4k}$

and asymptotic series

$\mathrm{b}\mathrm{e}\mathrm{r}(x)\sim \frac{e^{\frac{x}{\sqrt{2}}}}{\sqrt{2\pi x}}(f_1(x)\cos \alpha +g_1(x)\sin \alpha )-\frac{\mathrm{k}\mathrm{e}\mathrm{i}(x)}{\pi }$,

where

$\alpha =\frac{x}{\sqrt{2}}-\frac{\pi }{8},$

$f_1(x)=1+\sum _{k\ge 1}\frac{\cos (k\pi /4)}{k!(8x{)}^k}\prod _{l=1}^k(2l-1{)}^2$

$g_1(x)=\sum _{k\ge 1}\frac{\sin (k\pi /4)}{k!(8x{)}^k}\prod _{l=1}^k(2l-1{)}^2.$

Plot of the Kelvin function bei(z) in the complex plane from -2-2i to 2+2i with colors created with Mathematica 13.1 function ComplexPlot3D

Plot of the Kelvin function bei(z) in the complex plane from -2-2i to 2+2i with colors created with Mathematica 13.1 function ComplexPlot3D

bei(x)

File:Mplwp Kelvin-bei.svg

bei(x) for x between 0 and 20.

File:Mplwp Kelvin-bei-norm.svg

$\mathrm{b}\mathrm{e}\mathrm{i}(x)/e^{x/\sqrt{2}}$ for x between 0 and 50.

For integers n, bei_n(x) has the series expansion

${\mathrm{b}\mathrm{e}\mathrm{i}}_n(x)={\left(\frac{x}{2}\right)}^n\sum _{k\ge 0}\frac{\sin \left[(\frac{3n}{4}+\frac{k}{2})\pi \right]}{k!\Gamma (n+k+1)}{\left(\frac{x^2}{4}\right)}^k.$

The special case bei₀(x), commonly denoted as just bei(x), has the series expansion

Plot of the Kelvin function ker(z) in the complex plane from -2-2i to 2+2i with colors created with Mathematica 13.1 function ComplexPlot3D

Plot of the Kelvin function ker(z) in the complex plane from -2-2i to 2+2i with colors created with Mathematica 13.1 function ComplexPlot3D

$\mathrm{b}\mathrm{e}\mathrm{i}(x)=\sum _{k\ge 0}\frac{(-1{)}^k}{[(2k+1)!{]}^2}{\left(\frac{x}{2}\right)}^{4k+2}$

and asymptotic series

$\mathrm{b}\mathrm{e}\mathrm{i}(x)\sim \frac{e^{\frac{x}{\sqrt{2}}}}{\sqrt{2\pi x}}[f_1(x)\sin \alpha -g_1(x)\cos \alpha ]-\frac{\mathrm{k}\mathrm{e}\mathrm{r}(x)}{\pi },$

where α, $f_1(x)$, and $g_1(x)$ are defined as for ber(x).

ker(x)

File:Mplwp Kelvin-ker.svg

ker(x) for x between 0 and 14.

File:Mplwp Kelvin-ker-norm.svg

$\mathrm{k}\mathrm{e}\mathrm{r}(x)e^{x/\sqrt{2}}$ for x between 0 and 50.

For integers n, ker_n(x) has the (complicated) series expansion

$\begin{array}{cc}& {\mathrm{k}\mathrm{e}\mathrm{r}}_n(x)=-\ln \left(\frac{x}{2}\right){\mathrm{b}\mathrm{e}\mathrm{r}}_n(x)+\frac{\pi }{4}{\mathrm{b}\mathrm{e}\mathrm{i}}_n(x)\\ & +\frac{1}{2}{\left(\frac{x}{2}\right)}^{-n}\sum _{k=0}^{n-1}\cos \left[(\frac{3n}{4}+\frac{k}{2})\pi \right]\frac{(n-k-1)!}{k!}{\left(\frac{x^2}{4}\right)}^k\\ & +\frac{1}{2}{\left(\frac{x}{2}\right)}^n\sum _{k\ge 0}\cos \left[(\frac{3n}{4}+\frac{k}{2})\pi \right]\frac{\psi (k+1)+\psi (n+k+1)}{k!(n+k)!}{\left(\frac{x^2}{4}\right)}^k.\end{array}$

Plot of the Kelvin function kei(z) in the complex plane from -2-2i to 2+2i with colors created with Mathematica 13.1 function ComplexPlot3D

Plot of the Kelvin function kei(z) in the complex plane from -2-2i to 2+2i with colors created with Mathematica 13.1 function ComplexPlot3D

The special case ker₀(x), commonly denoted as just ker(x), has the series expansion

$\mathrm{k}\mathrm{e}\mathrm{r}(x)=-\ln \left(\frac{x}{2}\right)\mathrm{b}\mathrm{e}\mathrm{r}(x)+\frac{\pi }{4}\mathrm{b}\mathrm{e}\mathrm{i}(x)+\sum _{k\ge 0}(-1{)}^k\frac{\psi (2k+1)}{[(2k)!{]}^2}{\left(\frac{x^2}{4}\right)}^{2k}$

and the asymptotic series

$\mathrm{k}\mathrm{e}\mathrm{r}(x)\sim \sqrt{\frac{\pi }{2x}}{e}^{-\frac{x}{\sqrt{2}}}[f_2(x)\cos \beta +g_2(x)\sin \beta ],$

where

$\beta =\frac{x}{\sqrt{2}}+\frac{\pi }{8},$

$f_2(x)=1+\sum _{k\ge 1}(-1{)}^k\frac{\cos (k\pi /4)}{k!(8x{)}^k}\prod _{l=1}^k(2l-1{)}^2$

$g_2(x)=\sum _{k\ge 1}(-1{)}^k\frac{\sin (k\pi /4)}{k!(8x{)}^k}\prod _{l=1}^k(2l-1{)}^2.$

kei(x)

File:Mplwp Kelvin-kei.svg

kei(x) for x between 0 and 14.

File:Mplwp Kelvin-kei-norm.svg

$\mathrm{k}\mathrm{e}\mathrm{i}(x)e^{x/\sqrt{2}}$ for x between 0 and 50.

For integer n, kei_n(x) has the series expansion

$\begin{array}{cc}& {\mathrm{k}\mathrm{e}\mathrm{i}}_n(x)=-\ln \left(\frac{x}{2}\right){\mathrm{b}\mathrm{e}\mathrm{i}}_n(x)-\frac{\pi }{4}{\mathrm{b}\mathrm{e}\mathrm{r}}_n(x)\\ & -\frac{1}{2}{\left(\frac{x}{2}\right)}^{-n}\sum _{k=0}^{n-1}\sin \left[(\frac{3n}{4}+\frac{k}{2})\pi \right]\frac{(n-k-1)!}{k!}{\left(\frac{x^2}{4}\right)}^k\\ & +\frac{1}{2}{\left(\frac{x}{2}\right)}^n\sum _{k\ge 0}\sin \left[(\frac{3n}{4}+\frac{k}{2})\pi \right]\frac{\psi (k+1)+\psi (n+k+1)}{k!(n+k)!}{\left(\frac{x^2}{4}\right)}^k.\end{array}$

The special case kei₀(x), commonly denoted as just kei(x), has the series expansion

$\mathrm{k}\mathrm{e}\mathrm{i}(x)=-\ln \left(\frac{x}{2}\right)\mathrm{b}\mathrm{e}\mathrm{i}(x)-\frac{\pi }{4}\mathrm{b}\mathrm{e}\mathrm{r}(x)+\sum _{k\ge 0}(-1{)}^k\frac{\psi (2k+2)}{[(2k+1)!{]}^2}{\left(\frac{x^2}{4}\right)}^{2k+1}$

and the asymptotic series

$\mathrm{k}\mathrm{e}\mathrm{i}(x)\sim -\sqrt{\frac{\pi }{2x}}{e}^{-\frac{x}{\sqrt{2}}}[f_2(x)\sin \beta +g_2(x)\cos \beta ],$

where β, f₂(x), and g₂(x) are defined as for ker(x).

See also

• Bessel function

References

• .

External links

• Weisstein, Eric W. "Kelvin Functions." From MathWorld—A Wolfram Web Resource. [1]
• GPL-licensed C/C++ source code for calculating Kelvin functions at codecogs.com: [2]