Typos
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@ -168,7 +168,7 @@ Using Ohm's law and Kirchoff's law, calculate the effective resistance $R_{\text
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\pagebreak
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We can now use effective resistance to simplify complicated circuits. Whenever we see the above constructions
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(resistors in parellel or in series) in a graph, we can replace them with a single resistor of appropriate value.
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(resistors in parallel or in series) in a graph, we can replace them with a single resistor of appropriate value.
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\problem{}
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@ -243,13 +243,13 @@ If we place $A$ and $B$ at opposing vertices, what is the effective resistance o
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and $B$ at \texttt{111...1}. We can divide our cube into $n+1$ layers based on how many ones are in each
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node's binary string, with the $k^\text{th}$ layer having $k$ ones. By symmetry, all the nodes in each layer
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have the same voltage. This means we can think of the layers as connected in series, with the resistors
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inside each layer connected in parellel.
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inside each layer connected in parallel.
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\vspace{2mm}
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There are $\binom{n}{k}$ nodes in the $k^\text{th}$ layer. Each node in this layer has $k$ ones, so
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there are $n - k$ ways to flip a zero to get to the $(k + 1)^\text{th}$ layer. In total, there are
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$\binom{n}{k}(n - k)$ parellel connections from the $k^\text{th}$ layer to the $(k + 1)^\text{th}$
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$\binom{n}{k}(n - k)$ parallel connections from the $k^\text{th}$ layer to the $(k + 1)^\text{th}$
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layer, creating an effective resistance of
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$$
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\frac{1}{\binom{n}{k}(n - k)}
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