The Tellinen Everett component is a flux tube of fixed length and cross-sectional area that models ferromagnetic hysteresis based on the Tellinen model and the Everett function. The hysteresis curve is static and is determined by the parameters of the Everett function used by the magnetic material.

The Hysteresis Material parameter specifies a record of parameter values, it should be the instance name of a magnetic material from the palette Magnetic > Material > Hysteresis > Parameter Based. See Magnetic Material with Parameter-based Hysteresis.

The Use default material boolean parameter, when true, sets the Hysteresis Material parameter to hysteresisParameterMaterial1, which corresponds to the default name assigned to a record of the appropriate class. To use a different name, uncheck the box and enter the name for the parameter that appears.

$\{\left(T_{\mathrm{heatPort}}\=T\;\neg \mathrm{useHeatPort}\right)$

$\{\begin{array}{cc}\left\{\mathrm{dHyst}\=0\,k\=\frac{1}{100}\right\}& \mathrm{initial}\left(\right)\\ \left\{\mathrm{dHyst}\=\frac{d\left(-H_{\mathrm{stat}}{\mathrm{\mu }}_0\+\mathrm{hystR}\right)}{\mathrm{dt}}\,k\=\max \left(\frac{1}{100}\,\frac{\mathrm{hystF}-B}{\mathrm{diffHyst}}\right)\right\}& \mathrm{asc}\\ \left\{\mathrm{dHyst}\=\frac{d\left(-H_{\mathrm{stat}}{\mathrm{\mu }}_0\+\mathrm{hystF}\right)}{\mathrm{dt}}\,k\=\max \left(\frac{1}{100}\,\frac{B-\mathrm{hystR}}{\mathrm{diffHyst}}\right)\right\}& \mathrm{otherwise}\end{array}$

$H\=\frac{V_m}{l}$

$H\=H_{\mathrm{stat}}\+H_{\mathrm{eddy}}$

$H_2\=H_{\lim }-H_{c\left(\mathrm{mat}\right)}$

$H_3\=-H_{\lim }-H_{c\left(\mathrm{mat}\right)}$

$H_{\lim }\&equals;\{\begin{array}{cc}-H_{\mathrm{sat}\left(\mathrm{mat}\right)}& H_{\mathrm{stat}}<-H_{\mathrm{sat}\left(\mathrm{mat}\right)}\\ H_{\mathrm{sat}\left(\mathrm{mat}\right)}& H_{\mathrm{sat}\left(\mathrm{mat}\right)}<H_{\mathrm{stat}}\\ H_{\mathrm{stat}}& \mathrm{otherwise}\end{array}$

$H_{\mathrm{eddy}}\&equals;\{\begin{array}{cc}\mathrm{eddyCurrentFactor}\frac{\mathrm{dB}}{\mathrm{dt}}& \mathrm{includeEddyCurrents}\\ 0& \mathrm{otherwise}\end{array}$

$P_2\&equals;M_{\mathrm{mat}}{r}_{\mathrm{mat}}\left(\frac{2}{\mathrm{\pi }}\arctan \left(q_{\mathrm{mat}}{H}_2\right)\&plus;1\right)\&plus;2M_{\mathrm{mat}}\frac{1-r_{\mathrm{mat}}}{1\&plus;\frac{1}{2}\exp \left(-{\mathrm{p1}}_{\mathrm{mat}}{H}_2\right)\&plus;\frac{1}{2}\exp \left(-{\mathrm{p2}}_{\mathrm{mat}}{H}_2\right)}$

$P_3\&equals;M_{\mathrm{mat}}{r}_{\mathrm{mat}}\left(\frac{2}{\mathrm{\pi }}\arctan \left(q_{\mathrm{mat}}{H}_3\right)\&plus;1\right)\&plus;2M_{\mathrm{mat}}\frac{1-r_{\mathrm{mat}}}{1\&plus;\frac{1}{2}\exp \left(-{\mathrm{p1}}_{\mathrm{mat}}{H}_3\right)\&plus;\frac{1}{2}\exp \left(-{\mathrm{p2}}_{\mathrm{mat}}{H}_3\right)}$

$\mathrm{\Phi }\&equals;BA\&equals;{\mathrm{\Phi }}_p\&equals;-{\mathrm{\Phi }}_n$

$V_m\&equals;V_{m_p}-V_{m_n}$

$\mathrm{asc}\&equals;0<\frac{{\mathrm{dH}}_{\mathrm{stat}}}{\mathrm{dt}}$

$\mathrm{hystF}\&equals;J_s\&plus;\mathrm{unitT}\left(-P_1{P}_3\&plus;P_2{P}_4\right)\&plus;{\mathrm{\mu }}_0{H}_{\mathrm{stat}}\&plus;\frac{1}{2}\mathrm{eps}$

$\mathrm{hystR}\&equals;-J_s\&plus;\mathrm{unitT}\left(P_1{P}_2-P_3{P}_4\right)\&plus;{\mathrm{\mu }}_0{H}_{\mathrm{stat}}-\frac{1}{2}\mathrm{eps}$

$\mathrm{LossPower}\&equals;\mathrm{LossPowerStat}\&plus;\mathrm{LossPowerEddy}$

$\mathrm{LossPowerEddy}\&equals;H_{\mathrm{eddy}}\frac{\mathrm{dB}}{\mathrm{dt}}V$

$\mathrm{LossPowerStat}\&equals;H_{\mathrm{stat}}\frac{\mathrm{dB}}{\mathrm{dt}}V$

$\mathrm{diffHyst}\&equals;\mathrm{hystF}-\mathrm{hystR}$

$\frac{\mathrm{dB}}{\mathrm{dt}}\&equals;k\mathrm{dHyst}\&plus;{\mathrm{\mu }}_0\frac{{\mathrm{dH}}_{\mathrm{stat}}}{\mathrm{dt}}$

$\frac{\mathrm{dMagRel}}{\mathrm{dt}}\&equals;0$

The component described in this topic is from the Modelica Standard Library. To view the original documentation, which includes author and copyright information, click here.