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Poynting’s Theorem … energy conservation John Henry Poynting (1852-1914)

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Presentation on theme: "Poynting’s Theorem … energy conservation John Henry Poynting (1852-1914)"— Presentation transcript:

1 Poynting’s Theorem … energy conservation John Henry Poynting (1852-1914)

2 To recap… The energy stored in an electric field E is expressed as the work needed to “assemble” a group of point charges The energy stored in an electric field E is expressed as the work needed to “assemble” a group of point charges

3 Magnetic fields also store energy Magnetic fields also store energy Total energy stored by electromagnetic fields per unit volume is… Total energy stored by electromagnetic fields per unit volume is…

4 Work done moving a charge… Use the Lorentz formula: Use the Lorentz formula: The work in time-interval dt is then: The work in time-interval dt is then: (remember: Magnetic fields do no work!)

5 Remember current density J! The moving charge or charges constitute a current density, so we can write which means the work can now be expressed as Remember current density J! The moving charge or charges constitute a current density, so we can write which means the work can now be expressed as Remember that this is a rate of change of the energy (work) and so represents power delivered per unit volume

6 Now use Maxwell’s Equations And the identity

7 The “Work-Energy” Theorem for EM Fields… Poynting’s Theorem tells us: Poynting’s Theorem tells us: Change in energy stored in the fields Energy radiated across surface by the electromagnetic fields

8 The Poynting Vector


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