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Jackson solutions - jackson 6 9 homework solution, Provas de Física

Solução do jackson

Tipologia: Provas

2016

Compartilhado em 28/04/2016

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Jackson 6.9 Homework Problem Solution
Dr. Christopher S. Baird
University of Massachusetts Lowell
PROBLEM:
Discuss the conservation of energy and linear momentum for a macroscopic system of sources and
electromagnetic fields in a uniform, isotropic medium described by a permittivity ε and a permeability
μ. Show that in a straightforward calculation the energy density, Poynting vector, field-momentum
density, and Maxwell stress tensor are given by the Minkowski expressions:
u=1
2 E2 H2)
S=E×H
g ϵE×H
Tij=[ ϵ EiEj HiHj1
2δij( ϵ E2 H2)]
What modifications are made if ε and μ are functions of position?
SOLUTION:
As derived in class, the energy density and energy flux density in linear, low-dispersion, low-loss
materials are given by:
u=1
2
(
HB+ED
)
and
S=E×H
For linear material, B = μH and D = εE so these become:
u=1
2
(
ϵE2 H2
)
and
S=E×H
The field-momentum density is given by:
g=S
v2
In linear materials, the speed of the waves are given by
so that
g ϵ E×H
The Maxwell stress tensor describes the electromagnetic momentum flux and is given by:
pf2

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Jackson 6.9 Homework Problem Solution

Dr. Christopher S. Baird University of Massachusetts Lowell PROBLEM: Discuss the conservation of energy and linear momentum for a macroscopic system of sources and electromagnetic fields in a uniform, isotropic medium described by a permittivity ε and a permeability μ. Show that in a straightforward calculation the energy density, Poynting vector, field-momentum density, and Maxwell stress tensor are given by the Minkowski expressions: u =

E 2 +μ H 2 ) S = E × H g =μ ϵ E × H T (^) ij =[ϵ Ei E (^) jH (^) i H (^) j

δ ijE 2 +μ H 2 )] What modifications are made if ε and μ are functions of position? SOLUTION: As derived in class, the energy density and energy flux density in linear, low-dispersion, low-loss materials are given by: u =

( H ⋅ B + E ⋅ D ) and S = E × H

For linear material, B = μ H and D = ε E so these become: u =

( ϵ^ E

2 +μ H 2

) and S = E × H

The field-momentum density is given by: g =

S

v 2 In linear materials, the speed of the waves are given by v =^

√ ϵμ^

so that g =μ ϵ E × H The Maxwell stress tensor describes the electromagnetic momentum flux and is given by:

T (^) ij =[ϵ 0 Ei E (^) j +

μ 0 Bi B (^) j

δ ij (ϵ 0 E 2

μ 0

B

2 )] For linear materials, replace the permeability and permittivity of free space with the material's values: T (^) ij =[ϵ Ei E (^) j +

μ Bi B (^) j

δ ijE 2

μ

B

2 )] Switch out B for H using B = μ H T (^) ij =[ϵ Ei E (^) jH (^) i H (^) j

δ ijE 2 +μ H 2 )] Seeing as all of these equations are position-dependent densities, they automatically take into account the possibility of position-dependent permeabilities and permittivities. We do not need to change anything if ε and μ are functions of position. This is the advantage of working with densities instead of total values.