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_0rac{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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