At line 13 changed 1 line. |
|[{Math fontsize='14' latex='\\nabla\\times\\vec{H} = \\vec{J} + \\frac{\\partial \\vec{D}}{\\partial t}' }] | [{Math fontsize='14' |
!Ampéruv-Mawellův zákon |
At line 15 added 3 lines. |
[{MathInline fontsize='14' latex='\\nabla\\times\\vec{H} = \\vec{J} + \\frac{\\partial \\vec{D}}{\\partial t}' }] |
[{MathInline fontsize='14' |
|
At line 20 added 2 lines. |
Elektrický indukční tok je definován jako: |
|
At line 19 changed 1 line. |
|[{Math fontsize='14' latex='\\nabla\\times\\vec{E} = - \\frac{\\partial \\vec{B}}{\\partial t}' }] | [{Math fontsize='14' |
!Faradayův zákon |
At line 26 added 3 lines. |
[{MathInline fontsize='14' latex='\\nabla\\times\\vec{E} = - \\frac{\\partial \\vec{B}}{\\partial t}' }] |
[{MathInline fontsize='14' |
|
At line 31 added 2 lines. |
Magnetický indukční tok je definován jako: |
|
At line 25 changed 1 line. |
|[{Math fontsize='14' |
!Gaussův zákon pro elektrostatické pole |
At line 27 changed 1 line. |
\nabla\cdot\vec{D} = \rho_0 }] | [{Math fontsize='14' |
[{MathInline fontsize='14' latex='\\nabla\\cdot\\vec{D} = \\rho_0' }] |
[{MathInline fontsize='14' latex='\\oint_{S} \\vec{D}\\, d\\vec{S}=Q_0' }] |
At line 29 changed 1 line. |
\oint_{S} D\, dS=Q_0 }] |
!Gaussův zákon pro magnetické pole |
At line 31 changed 1 line. |
|[{Math fontsize='14' |
[{MathInline fontsize='14' latex='\\nabla\\cdot\\vec{B} = 0' }] |
[{MathInline fontsize='14' latex='\\oint_{S} \\vec{B}\\, d\\vec{S}=0' }] |
At line 33 removed 4 lines. |
\nabla\cdot\vec{B} = 0}] | [{Math fontsize='14' |
|
\oint_{S} B\, dS=0 }] |
|
At line 49 added 10 lines. |
|
!!Poyntinguv vektor |
|
Poyntingův vektor vyjadřuje okamžitou hodnotu plošné hustoty výkonu. Směr vektoru [{MathInline fontsize='12' latex='\\vec{S}'}], který |
je kolmý na [{MathInline fontsize='12' latex='\\vec{E}'}] a [{MathInline fontsize='12' latex='\\vec{H}'}] , udává směr toku energie. Je definován jako |
|
[{Math fontsize='12' |
|
\vec{S}=\vec{E}\times\vec{H} }] |
|