Optics SUB-MENU Optics Sub-menu Problem NoChaptersChapters


561.


Problem 41.31 (RHK)


A coaxial cable (inner radius a, outer radius b) is used as a transmission line between a battery and a resistance R, as shown in the figure. (a) We have to calculate E, B for ; (b) calculate the Poynting vector for ; (c) by suitably integrating the Poynting vector show that the total power flowing across the annular cross section is . We have to answer whether this is reasonable. (d) We have to show that the direction of is always from the battery to the resistor, no matter which way the battery is connected.


Solution:           Click For PDF Version

(a)

As the outer and the inner surfaces of the coaxial cable are connected to a battery of emf , the electric field inside the region between the two current carrying parts of the cable will be radial and of magnitude

where b is the outer radius and a is the inner radius of the cable.

As the cable forms a circuit with a resistor of resistance R connected to the battery, there will be a current flow of magnitude

Because of the current flow in the inner part of the coaxial cable and the cylindrical symmetry of the cable there will be a circular magnetic field about the axis of the cable of magnitude



(b)

The magnetic field vector and the electric field vector will be perpendicular to each other and it can be seen that will be parallel to the axis of cable pointing in the direction of the flow of current from the battery to the resistor. Therefore, the magnitude of at radial distance r from the axis of the cable will be

(c)

Integrating the Poynting vector over any annular cross section of the cable, we can obtain the power flowing inside the cable. We find

As

,

the power flowing inside the cable

is equal to the Joule dissipation of the energy by the resistor.