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Chapter 11 Radiation 11.1 Dipole Radiation 11.2 Point Charges.

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Presentation on theme: "Chapter 11 Radiation 11.1 Dipole Radiation 11.2 Point Charges."— Presentation transcript:

1 Chapter 11 Radiation 11.1 Dipole Radiation 11.2 Point Charges

2 11.1 Dipole Radiation 11.1.1 What is Radiation?
Electric Dipole Radiation

3 What is Radiation? The source of EM waves is from the radiation of accelerating charges and changing currents. The signature of radiation is the irreversible flow of energy away from the source. Assume that the source is localized near the origin. The total power passing out through the surface at radius r is The power radiated is For static fields, Static field does not radiate.

4 11.1.1 (2) But, Jefimenko’s equations: In the and terms,
These terms are responsible for EM radiation

5 11.1.2 Electric Dipole Radiation
approximation 1:

6 (2) approximation 2: approximation 3:

7 11.1.2 (3) Keep only zeroth order of [ approximation 1:

8 (4) [ approximation 3]

9 (5)

10 11.1.2 (6) The energy radiated by an oscillating electric dipole is
determined by the Poynting vector: The total power radiated is

11 11.1.2 (7) Example 11.1 (a) Why the sky is blue during the day ?
Answer : Sun’s radiation is white-light. The absorption of the white-light by the atmosphere atoms is more on higher frequency. The reradiation so more on the blue than the red. The sky is blue .

12 11.1.2 (8) (b)Why, during the sunset, the sky is more red ?
Longer, more scattering, especially for Blue lights.  more red-lights reach.

13 11.2 Point Charges The fields of a point charge q in arbitrary motion
Velocity field Acceleration field Radiation field The Poynting vector

14 11.2 (2) The radiation energy is the stuff that detaches itself from the charge and propagates off to infinity.  Only terms of remain (the terms ) That is, only the terms of survive.

15 11.2 (3)

16 11.2 (4) The total power radiated Larmor formula

17 11.2 (5) if Rate of gun shoot Rate of strike on the target

18 11.2 (6) The power radiated by the particle
The power radiated by the particle into per solid angle The total power radiated is Lienard`s generalization of the Larmor formula

19 11.2 (7) Example 11.3 Solution:

20 11.2 (8)

21 11.2 (9) The total power radiated Same radiation result.

22 11.2 (10) producting radiation (or photon) (bremsstrahlung)
(annilation) Prob synchrotron radiation


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