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Commit 5cafb70b authored by Erik Strand's avatar 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?
$$
\begin{align*}
Z &= \sqrt{\frac{L}{C}} \\
&= \sqrt{\frac{\mu_0}{2 \pi} \ln \left( \frac{r_o}{r_i} \right)
\frac{1}{2 \pi \epsilon_0 \epsilon_r} \ln \left( \frac{r_o}{r_i} \right)} \\
&= \frac{1}{2 \pi} \sqrt{\frac{\mu_0}{\epsilon_0 \epsilon_r}} \ln \left( \frac{r_o}{r_i} \right) \\
&= 51.6 \si{\ohm}
\end{align*}
$$
### (b) ### (b)
{:.question} {:.question}
What is the velocity? What is the velocity?
$$
\begin{align*}
v &= \frac{1}{\sqrt{L C}} \\
&= \frac{1}{\sqrt{\frac{\mu_0 \ln(r_o / r_i)}{2 \pi}
\frac{2 \pi \epsilon_0 \epsilon_r}{\ln( r_o / r_i )}}} \\
&= \frac{1}{\sqrt{\mu_0 \epsilon_0 \epsilon}} \\
&= \num{2e8} \si{m/s}
\end{align*}
$$
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?
$$
\num{1e-9} \si{s} \cdot \num{2e8} \si{m/s} = 0.2 \si{m}
$$
### (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 $$r_i$$,
$$
r_i = r_0 \cdot e^{-2 \pi \cdot 51.6 \sqrt{\epsilon_0 \epsilon_r / \mu_0}}
$$
### (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 $$\lambda \nu = c$$, so
$$
\num{2e8} \si{m/s} \cdot \frac{1}{2 \cdot \num{1.48e-3} \si{m}} = \num{6.76e10} \si{Hz}
$$
## (7.6) ## (7.6)
......
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