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This is chapter 21, problem number 92.
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Q factor can be defined as the voltage across a capacitor or an inductor, the voltage across a resistor at resonance.
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The larger, the q factor is the sharper the resonance car will be.
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In part a, they want us to show that the q factor is given by 1 over r square root of l over c, the inductance over capacitance.
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So we know the definition of q.
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It's given to us in the problem.
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It's either the potential across the capacitor over the potential across the resistor, or you could use the potential across the inductor over the potential across the resistor.
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So both are valid.
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Both are going to take you to the correct answer.
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Let me pick the first one here.
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Now, the potential across the capacitor is at the resonant, then we have the resin current times the reactance of the capacitor, right? where we know that the reactants of the capacitor is 1 over 2 pi -f capacitance.
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So i'm just going to put everything back in this equation.
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So the q factor is going to be equal to i, resident, and s.
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Xc, which is, right, let's write it, one over 2xfc.
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And in denominator, i still have 1 over times 1 over vr, right? br, as you know from olm's law, is going to be the i resonite, right, times the resistance.
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Now, i resonant and then times resistant.
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So the currents are going to cancel chitter out, the q factor is going to be 1 over 2 pi f, c .r.
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Now i want to pay attention to what f really is.
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F is the resonant frequency, and it's given to us as 1 over 2 pi, 1 over out of time c, if you remember this equation.
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Now, when that's the case, then let's plus.
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In for f in the q factor equation, right? so i'm rewriting the q factor equals then 1 over 2 pi times f, which is 1 over 2 pi square root of 1 over l .c times c times r, right? so 2 pies are going to cancel each other out.
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What we have then is 1 over square root of 1.
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L times c times c r.
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Let's put the c back in the square root.
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Then we're going to have to take the square of it, right? so it's going to be equal to one instead of one...