Exam 2 extra credit hints
We know reactances add like resistances. The whole circuit has L and C in parallel, and that combination in series with a resistance. The total reactance is then $X_{tot} = X_R + X_{L||C}$, where $X_{L||C}$ is the reactance of the capacitor and inductor in parallel, which you'd find by adding the $L$ and $C$ reactances like you would parallel resistors. The resistor's reactance is just $X_R=R$. The current in the circuit is then the input voltage divided by the total reactance, $I=V_{in}/X_{tot}$.
What is the output voltage? You're measuring the output voltage across the $L$ and $C$ parallel combination, so it must be $V_{out}=IX_{L||C}$. Find the equivalent reactance of $L$ and $C$ in parallel, add the resistor's reactance, and you have the total reactance. That gets you the current, and the current times the equivalent reactance of $L$ and $C$ in parallel gives you the output. This will all be a function of frequency as well as $R$, $L$, and $C$.
Qualitatively, you can ignore the $L$ and $C$ one at a time. Without the $C$, it is a high-pass. Without the $L$, it is a low-pass. The whole circuit looks like a combination of the two - hates both high and low frequencies, but will like a middle range in between.
To sketch the plot, presume some values for $R$, $L$, and $C$. I would say perhaps $R\!=\!100\,\Omega$, $L\!=\!1\,$mH, and $C\!=\!1\,\mu$F. What is it good for? Any time you want to let a small range of frequencies through, but nothing else. Radio comes to mind.
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