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Write out Maxwell\'s Equations component wise in cylindrical coordinates in thei

ID: 1913954 • Letter: W

Question

Write out Maxwell's Equations component wise in cylindrical coordinates in their most general form. Remember that each field component can be a function of all three spatial dimensions as well as time. You should end up with eight equations: the two divergence equations, and three equations for the curl equations when they are separated component wise. At this point, assume that all source terms are present-that there exists both a charge density and a current density throughout the region of interest. This is the form you would need if you had to solve a fully general program for a wave form on a coaxial cable.

Explanation / Answer

First, the two divergence equations:

( abla . ec{B}=0)

thus, ( rac{1}{s} rac{partial s B_{s}}{partial s}+ rac{1}{s} rac{partial B_{phi}}{partial phi}+ rac{partial B_z}{partial z}=0)

Then,

( abla . ec{E}= ho/epsilon_0)

thus, ( rac{1}{s} rac{partial s E_{s}}{partial s}+ rac{1}{s} rac{partial E_{phi}}{partial phi}+ rac{partial E_z}{partial z}= ho/epsilon_0)

Now, curl equations:

( abla imes ec{E}=- rac{partial ec{B}}{partial t})

Thus,

(left({1 over ho}{partial E_z over partial phi}    - {partial E_phi over partial z} ight)=-{partial B_{ ho} over partial ho})

(left({partial E_ ho over partial z} - {partial E_z over partial ho} ight)=-{partial B_{phi} over partial phi})

(left({partial left( ho E_phi ight) over partial ho} - {partial E_ ho over partial phi} ight)=-{partial B_{z} over partial z})

Also,

( abla imes ec{B}=mu_0 ec{J}+mu_0 u_0 rac{partial ec{E}}{partial t})

Thus,

(left({1 over ho}{partial B_z over partial phi}    - {partial B_phi over partial z} ight)=mu_0 J_ ho+mu_0 u_0{partial E_{ ho} over partial ho})

(left({partial B_ ho over partial z} - {partial B_z over partial ho} ight)=mu_0 J_phi+mu_0 u_0{partial E_{phi} over partial phi})

(left({partial left( ho B_phi ight) over partial ho} - {partial B_ ho over partial phi} ight)=mu_0 J_z+mu_0 u_0{partial E_{z} over partial z})

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