Radiation mechanism in dipole:
Consider a small dipole antenna where the time of travel is negligible.
Consider a small dipole antenna where the time of travel is negligible.
fig 1a. at a quarter -wavelength 1b. at half-wavelength(opposite charges) 1c. at half-wavelength (no charge on the conductor) |
Consider that a small dipole is center-fed in the first quarter of the period T i.e., t=T/4 , at this time the charge attains maximum value. At this instant, the lines travel radially outwards at a distance of . Assume that the number of lines produced is three as shown in fig., 1a above
Now in the next quarter period of time, three lines produced originally, travel an additional distance of . So the total distance becomes . The charge density on the conductor starts diminishing as the opposite charges are introduced. These opposite charges neutralize the charges on the conductor and they also produce three lines of force which travel a distance of during the second quarter of the first half. The lines of force produced by the opposite charges are as shown by the dashed lines as shown above in fig., 1b
As compared with the lines of force in the first quarter of the first half, the direction of lines of force is opposite (i.e., upwards) as they are produced by opposite charges. As a result, the appearance of the three lines of force directing upwards in the first distance while three more lines of force directing downwards in the next distance. Now there is no charge on the conductor, the lines of force get detached from conductors and combine to form closed loops as shown in fig., 1c above.
It is obvious that in the second half of the period the same procedure is carried out but in the opposite direction. The process is then repeated and carried out indefinitely.
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