Answered: 1 °B(は,t)= -v²B(ï,t) | bartleby

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Using only Maxwell's equations in vacuum and vector identities, show that the magnetic field also satisfies the wave equation:

B(ï,t)
1
V²B(ï,t).

Note: Remember that Maxwell's equations in vacuum are:
0,
Gauss's law for the electric field
(186)
0,
Gauss's law for the magnetic field
(187)
Faraday's Law
(188)
dt
Ampère-Maxwell Law
(189)
Ət

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