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Using the appropriate theorems from vector calculus, starting from their time-dependent differential form, derive the integral form of the following two equations in Maxwell’s equations. You must clearly explain your working and reasoning. a) ∇×B−(mu)0(epsilon)0((delta)E/(delta)t)=(mu)0j b) ∇⋅E=(rho)/(epsilon)0

Using the appropriate theorems from vector calculus, starting from their time-dependent differential form, derive the integral form of the following two equations in Maxwell’s equations. You must clearly explain your working and reasoning. a) ∇×B−(mu)0(epsilon)0((delta)E/(delta)t)=(mu)0j b) ∇⋅E=(rho)/(epsilon)0

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Using the appropriate theorems from vector calculus, starting from their time-dependent differential form, derive the integral form of the following two equations in Maxwell’s equations. You must clearly explain your working and reasoning.
a) ∇×B−(mu)0(epsilon)0((delta)E/(delta)t)=(mu)0j
b) ∇⋅E=(rho)/(epsilon)0

Using the appropriate theorems from vector calculus, starting from their time-dependent differential form, derive the integral form of the following two equations in Maxwell's equations. You must clearly explain your working and reasoning. ƏE a) V× B – µloEo at = Hoj b) V·E = L Eo
Transcribed Image Text:Using the appropriate theorems from vector calculus, starting from their time-dependent differential form, derive the integral form of the following two equations in Maxwell's equations. You must clearly explain your working and reasoning. ƏE a) V× B – µloEo at = Hoj b) V·E = L Eo
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