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Erik Strand
pit
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d5322149
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d5322149
authored
6 years ago
by
Erik Strand
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Answer 6.6
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@@ -278,8 +278,63 @@ Assume that sunlight has a power energy density of $$1 \si{kW/m^2}$$ (this is a
typical average value in the continental USA is $$
\a
pprox 200
\s
i{W/m^2}$$). Estimate the electric
field strength associated with this radiation.
The energy delivered per square meter in one second by sunlight is the field energy stored in a 1
meter by 1 meter by 1 light second volume. So the average energy density of sunlight must be
$$
\f
rac{10^3
\s
i{J}}{1
\s
i{m}
\c
dot 1
\s
i{m}
\c
dot
\n
um{3e8}
\s
i{m}} =
\n
um{0.33e-5}
\s
i{J/m^3}
$$
The energy density of light in a vacuum is
$$
\b
egin{align
*
}
U &=
\f
rac{1}{2} (E
\c
dot D + B
\c
dot H)
\\
&=
\f
rac{1}{2}
\l
eft(
\e
psilon_0 |E|^2 +
\m
u_0 |H|^2
\r
ight)
\\
&=
\f
rac{1}{2}
\l
eft(
\e
psilon_0 |E|^2 +
\e
psilon_0 |E|^2
\r
ight)
\\
&=
\e
psilon_0 |E|^2
\e
nd{align
*
}
$$
since $$
\v
ert E
\v
ert /
\v
ert H
\v
ert =
\s
qrt{
\m
u_0/
\e
psilon_0}$$.
Thus the root mean square magnitude of the electric field must be
$$
\f
rac{
\n
um{0.33e-5}
\s
i{J/m^3}}{
\e
psilon_0} =
\n
um{3.8e5}
\s
i{V^2/m^2}
$$
Since the electric field is a sinusoidal wave, the root mean square amplitude is half the maximum
amplitude. So the peak field strength is $$
\n
um{7.5e5}
\s
i{V/m}$$.
### (b)
{:.question}
If 1 W of power is focused in a laser beam to a square millimeter, what is the field strength? What
about if it is focused to the diffraction limit of $$
\a
pprox 1
\s
i{
\m
u m^2}$$?
Summarizing the previous section, we found that the root mean square field strength necessary to
deliver $$x$$ watts of power to an area $$A$$ is
$$
\f
rac{x
\s
i{W}}{c
\s
i{m/s}}
\c
dot
\f
rac{1}{A
\s
i{m^2}}
\c
dot
\f
rac{1}{
\e
psilon_0
\s
i{F/m}}
$$
So for one watt to be delivered to a square millimeter, the RMS field strength is
$$
\f
rac{1
\s
i{W}}{
\n
um{3e8}
\s
i{m/s}}
\c
dot
\f
rac{1}{10^{-6}
\s
i{m^2}}
\c
dot
\f
rac{1}{
\n
um{8.85e-12}
\s
i{F/m}}
=
\n
um{3.8e8}
\s
i{V^2/m^2}
$$
which means the peak field strength is $$
\n
um{7.5e8}
\s
i{V/m}$$.
If it's focused down to a square micrometer, the RMS field strength is
$$
\f
rac{1
\s
i{W}}{
\n
um{3e8}
\s
i{m/s}}
\c
dot
\f
rac{1}{10^{-12}
\s
i{m^2}}
\c
dot
\f
rac{1}{
\n
um{8.85e-12}
\s
i{F/m}}
=
\n
um{3.8e14}
\s
i{V^2/m^2}
$$
and the peak field strength is $$
\n
um{7.5e14}
\s
i{V/m}$$.
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