Chapter 24 Classical Theory of Electromagnetic Radiation A

  • Slides: 21
Download presentation
Chapter 24 Classical Theory of Electromagnetic Radiation

Chapter 24 Classical Theory of Electromagnetic Radiation

A. A charge at rest makes a 1/r 2 electric field but no magnetic

A. A charge at rest makes a 1/r 2 electric field but no magnetic field B. A charge moving with constant velocity makes a 1/r 2 electric field and 1/r 2 magnetic field C. An accelerated charge in addition makes electromagnetic radiation, with 1/r electric field and 1/r magnetic field.

Question A narrow collimated pulse of radiation propagates in the -x direction. There is

Question A narrow collimated pulse of radiation propagates in the -x direction. There is an electron at location A. What is the direction of the radiative electric field observed at location B? A e- D B C

Stability of Atoms Circular motion: Is there radiation emitted? Classical physics says “YES” Þ

Stability of Atoms Circular motion: Is there radiation emitted? Classical physics says “YES” Þ orbiting particle must lose energy! Þ speed decreases Þ particle comes closer to center Classical model of atom: Electrons should fall on nucleus! To explain the facts - introduction of quantum mechanics: Electrons can move around certain orbits only and emit E/M radiation only when jumping from one orbit to another v a

Undulator 1: magnets 2: electron beam entering from the upper left 3: synchrotron radiation

Undulator 1: magnets 2: electron beam entering from the upper left 3: synchrotron radiation exiting to the lower right If the oscillations are confined to a plane the radiation will be linearly polarized. If the oscillation trajectory is helical, the radiation will be circularly polarized, with the handedness determined by the helix.

History Accelerator-based synchrotron light was seen for the first time at the General Electric

History Accelerator-based synchrotron light was seen for the first time at the General Electric Research Laboratory in the USA in 1947 in a type of accelerator known as a synchrotron. First considered a nuisance because it caused the particles to lose energy, it recognized in the 1960 s as light with exceptional properties. Simply trillion times brighter than the beam produced by a hospital x-ray machine. Looking head on into the upper and lower rows of magnets (jaws) in an undulator. The adjustable vertical distance between the jaws determines the wavelength emitted. Here, a laser is used to simulate the burst of light produced. (Courtesy: Advanced Light Source)

Argonne National Laboratory, USA

Argonne National Laboratory, USA

Sinusoidal Electromagnetic Radiation Acceleration: Sinusoidal E/M field

Sinusoidal Electromagnetic Radiation Acceleration: Sinusoidal E/M field

Sinusoidal E/M Radiation: Wavelength Instead of period can use wavelength: Example of sinusoidal E/M

Sinusoidal E/M Radiation: Wavelength Instead of period can use wavelength: Example of sinusoidal E/M radiation: atoms radio stations E/M noise from AC wires Freeze picture in time:

Energy and Momentum of E/M Radiation According to particle theory of light: photons have

Energy and Momentum of E/M Radiation According to particle theory of light: photons have energy and momentum Classical E/M model of light: E/M radiation must carry energy and momentum

Energy of E/M Radiation A particle will experience electric force during a short time

Energy of E/M Radiation A particle will experience electric force during a short time d/c: What will happen to the ball? It will oscillate Energy was transferred from E/M field to the ball Amount of energy in the pulse is ~ E 2

Energy of E/M Radiation Ball gained energy: Pulse energy must decrease E/M radiation: E=c.

Energy of E/M Radiation Ball gained energy: Pulse energy must decrease E/M radiation: E=c. B Energy density of magnetic field in a traveling wave is exactly the energy density of the electric field

Energy Flux There is E/M energy stored in the pulse: Pulse moves in space:

Energy Flux There is E/M energy stored in the pulse: Pulse moves in space: there is energy flux Units: J/(m 2 s) = W/m 2 During t: used: E=c. B, 0 0=1/c 2

Energy Flux: The Poynting Vector The direction of the E/M radiation was given by

Energy Flux: The Poynting Vector The direction of the E/M radiation was given by Energy flux, the “Poynting vector”: John Henry Poynting (1852 -1914) • S is the rate of energy flux in E/M radiation • It points in the direction of the E/M radiation

Exercise A laser pointer emits ~5 m. W of light power. What is the

Exercise A laser pointer emits ~5 m. W of light power. What is the approximate magnitude of the electric field? Solution: 1. Spot size: ~2 mm 2. flux = (5. 10 -3 W)/(3. 14. 0. 0012 m 2)=1592 W/m 2 3. Electric field: (rms value) What if we focus it into 2 a micron spot? Flux will increase 106 times, E will increase 103 times:

Momentum of E/M Radiation • E field starts motion, • No net momentum change

Momentum of E/M Radiation • E field starts motion, • No net momentum change in the y direction • Moving charge in magnetic field: y x Fmag What if there is negative charge? ‘Radiation pressure’: What is its magnitude? Average speed: v/2 Fmag

Momentum Flux Net momentum: in transverse direction: 0 in longitudinal direction: >0 Relativistic energy:

Momentum Flux Net momentum: in transverse direction: 0 in longitudinal direction: >0 Relativistic energy: Quantum view: light consists of photons with zero mass: Classical (Maxwell): it is also valid, i. e. momentum = energy/speed Momentum flux: Units of Pressure

Exercise: Solar Sail What is the force due to sun light on a sail

Exercise: Solar Sail What is the force due to sun light on a sail with the area 1 km 2 near the Earth orbit (1400 W/m 2)? Solution: Note: What if we have a reflective surface? Total force on the sail: Atmospheric pressure is ~ 105 N/m 2

Re-radiation: Scattering Positive charge Electric fields are not blocked by matter: how can E

Re-radiation: Scattering Positive charge Electric fields are not blocked by matter: how can E decrease?

Cardboard Why there is no light going through a cardboard? Electric fields are not

Cardboard Why there is no light going through a cardboard? Electric fields are not blocked by matter Electrons and nucleus in cardboard reradiate light Behind the cardboard reradiated E/M field cancels original field

In which of these situations will the bulb light? A) B) C) D) E)

In which of these situations will the bulb light? A) B) C) D) E) A B C None B and C