e.m. field of charge in rectilinear motion I Start with Maxwells - - PowerPoint PPT Presentation

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e.m. field of charge in rectilinear motion I Start with Maxwells - - PowerPoint PPT Presentation

e.m. field of charge in rectilinear motion I Start with Maxwells equations Lets work out our way to an equation for A and P. Piot, PHYS 571 Fall 2007 e.m. field of charge in rectilinear motion II Using we get:


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SLIDE 1
  • P. Piot, PHYS 571 – Fall 2007

e.m. field of charge in rectilinear motion I

  • Start with Maxwell’s equations
  • Let’s work out our way to an equation for A and Φ
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SLIDE 2
  • P. Piot, PHYS 571 – Fall 2007
  • Using

we get:

  • In the Lorenz’ Gauge:
  • Thus
  • Using

gives

e.m. field of charge in rectilinear motion II

[JDJ 6.16] [JDJ 6.15] Inhomogeneous wave equations

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SLIDE 3
  • P. Piot, PHYS 571 – Fall 2007

e.m. field of charge in rectilinear motion III

  • So the problem is to solve the equation for A and Φ given the form
  • f ρ and J
  • For a moving charge distribution with velocity v

      − − =       Α Φ       ∂ ∂ − ∇ J t r r µ µε

ε ρ 2 2 2

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SLIDE 4
  • P. Piot, PHYS 571 – Fall 2007

e.m. field of charge in rectilinear motion IV

  • For both A and Φ we have to solve an inhomogeneous d’Alembert

equation of the form

  • Consider
  • Then
  • So

with

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SLIDE 5
  • P. Piot, PHYS 571 – Fall 2007

e.m. field of charge in rectilinear motion V

  • ….
  • Then our d’Alembert equation has the form
  • Consider a point charge
  • Vector potential is along z
  • And we have to solve
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SLIDE 6
  • P. Piot, PHYS 571 – Fall 2007

e.m. field of charge in rectilinear motion VI

  • The equation

is solve by inspection from

  • The results are
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SLIDE 7
  • P. Piot, PHYS 571 – Fall 2007

e.m. field of charge in rectilinear motion VII

  • The E-field can be calculated from
  • Which gives
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SLIDE 8
  • P. Piot, PHYS 571 – Fall 2007

e.m. field of charge in rectilinear motion VIII

  • In spherical coordinate
  • So
  • and
  • In vacuum
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SLIDE 9
  • P. Piot, PHYS 571 – Fall 2007

e.m. field of charge in rectilinear motion IX

  • Consider
  • Note that

the field line are squashed long the direction of motion.

E-field line associated to a moving charge with Lorentz factor γ

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SLIDE 10
  • P. Piot, PHYS 571 – Fall 2007

e.m. field of charge in rectilinear motion X

  • B- field can also be computed
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SLIDE 11
  • P. Piot, PHYS 571 – Fall 2007

e.m. field of charge in rectilinear motion XI

  • Further reduction (try to introduce an impact parameter b)
  • introducing

b x

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SLIDE 12
  • P. Piot, PHYS 571 – Fall 2007

e.m. field of charge in rectilinear motion XII

  • Example of E-field associated to a charge at rest (γ=1)and moving

with γ=10.

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SLIDE 13
  • P. Piot, PHYS 571 – Fall 2007

Space charge effects I

  • Let’s consider the interaction of two particle moving at parallel to

each other and consider the force experience by the particle of charge q0 from the other particle

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SLIDE 14
  • P. Piot, PHYS 571 – Fall 2007

Space charge effects II

  • Let’s consider the fields are generated by a source particle of unit

charge then