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Problem 5.39 In terms of the dc current I , how much magnetic energy is stored in the insulating medium of a 3-m-long, air-filled section of a coaxial transmission line, given that the radius of the inner conductor is 5 cm and the inner radius of the outer conductor is 10 cm? Solution: From Eq. (5.99), the inductance per unit length of an air-filled coaxial cable is given by L = μ 0 2π ln b a (H/m). Over a length of 2 m, the inductance is L = 2L = 3 × 4π × 10 7 2π ln 10 5 = 416 × 10 9 (H). From Eq. (5.104), W m = LI 2 /2 = 208I 2 (nJ), where W m is in nanojoules when I is in amperes. Alternatively, we can use Eq. (5.106) to compute W m : W m = 1 2 V μ 0 H 2 d V . From Eq. (5.97), H = B/μ 0 = I /2π r, and W m = 1 2 3m z=0 2π φ =0 b r=a μ 0 I 2π r 2 rdrd φ dz = 208I 2 (nJ).

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Problem 5.39 In terms of the dc currentI, how much magnetic energy is stored inthe insulating medium of a 3-m-long, air-filled section of a coaxial transmission line,given that the radius of the inner conductor is 5 cm and the inner radius ofthe outerconductor is 10 cm?

Solution: From Eq. (5.99), the inductance per unit length of an air-filled coaxialcable is given by

L′ =µ0

2πln

(

ba

)

(H/m).

Over a length of 2 m, the inductance is

L = 2L′ =3×4π×10−7

2πln

(

105

)

= 416×10−9 (H).

From Eq. (5.104),Wm = LI2/2 = 208I2 (nJ), whereWm is in nanojoules whenI is inamperes. Alternatively, we can use Eq. (5.106) to computeWm:

Wm =12

V

µ0H2 dV .

From Eq. (5.97),H = B/µ0 = I/2πr, and

Wm =12

∫ 3m

z=0

∫ 2π

φ=0

∫ b

r=aµ0

(

I2πr

)2

r dr dφdz = 208I2 (nJ).