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Erik Strand
pit
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5cafb70b
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5cafb70b
authored
6 years ago
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Erik Strand
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Answer 7.5
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...
@@ -125,17 +125,43 @@ inner radius of 0.406 mm, and an outer radius of 1.48 mm.
...
@@ -125,17 +125,43 @@ inner radius of 0.406 mm, and an outer radius of 1.48 mm.
{:.question}
{:.question}
What is the characteristic impedance?
What is the characteristic impedance?
$$
\b
egin{align
*
}
Z &=
\s
qrt{
\f
rac{L}{C}}
\\
&=
\s
qrt{
\f
rac{
\m
u_0}{2
\p
i}
\l
n
\l
eft(
\f
rac{r_o}{r_i}
\r
ight)
\f
rac{1}{2
\p
i
\e
psilon_0
\e
psilon_r}
\l
n
\l
eft(
\f
rac{r_o}{r_i}
\r
ight)}
\\
&=
\f
rac{1}{2
\p
i}
\s
qrt{
\f
rac{
\m
u_0}{
\e
psilon_0
\e
psilon_r}}
\l
n
\l
eft(
\f
rac{r_o}{r_i}
\r
ight)
\\
&= 51.6
\s
i{
\o
hm}
\e
nd{align
*
}
$$
### (b)
### (b)
{:.question}
{:.question}
What is the velocity?
What is the velocity?
$$
\b
egin{align
*
}
v &=
\f
rac{1}{
\s
qrt{L C}}
\\
&=
\f
rac{1}{
\s
qrt{
\f
rac{
\m
u_0
\l
n(r_o / r_i)}{2
\p
i}
\f
rac{2
\p
i
\e
psilon_0
\e
psilon_r}{
\l
n( r_o / r_i )}}}
\\
&=
\f
rac{1}{
\s
qrt{
\m
u_0
\e
psilon_0
\e
psilon}}
\\
&=
\n
um{2e8}
\s
i{m/s}
\e
nd{align
*
}
$$
This is two thirds the speed of light.
### (c)
### (c)
{:.question}
{:.question}
If a computer has a clock speed of 1 ns, how long can a length of RG58/U be and still deliver a
If a computer has a clock speed of 1 ns, how long can a length of RG58/U be and still deliver a
pulse within one clock cycle?
pulse within one clock cycle?
$$
\n
um{1e-9}
\s
i{s}
\c
dot
\n
um{2e8}
\s
i{m/s} = 0.2
\s
i{m}
$$
### (d)
### (d)
{:.question}
{:.question}
...
@@ -143,12 +169,24 @@ It is often desirable to use thinner coaxial cable to minimize size or weight bu
...
@@ -143,12 +169,24 @@ It is often desirable to use thinner coaxial cable to minimize size or weight bu
impedance of RG58/U (to minimize reflections). If such a cable has an outer diameter of 30 mils (a
impedance of RG58/U (to minimize reflections). If such a cable has an outer diameter of 30 mils (a
mil is a thousandth of an inch), what is the inner diameter?
mil is a thousandth of an inch), what is the inner diameter?
Solving the formula above for $$r_i$$,
$$
r_i = r_0
\c
dot e^{-2
\p
i
\c
dot 51.6
\s
qrt{
\e
psilon_0
\e
psilon_r /
\m
u_0}}
$$
### (e)
### (e)
{:.question}
{:.question}
For RG58/U, at what frequency does the wavelength become comparable to
For RG58/U, at what frequency does the wavelength become comparable to
the diameter?
the diameter?
We know $$
\l
ambda
\n
u = c$$, so
$$
\n
um{2e8}
\s
i{m/s}
\c
dot
\f
rac{1}{2
\c
dot
\n
um{1.48e-3}
\s
i{m}} =
\n
um{6.76e10}
\s
i{Hz}
$$
## (7.6)
## (7.6)
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