The Anatomy of a Resonant Circuit
Imagine a circuit where energy dances back and forth between an inductor and a capacitor, perfectly in sync with an external alternating voltage. This is the magic of a resonance circuit. In this problem, we are given a circuit oscillating at a resonant frequency of f0=10 MHz, which is 107 Hz.
The circuit features an inductor with an inductance of L=2×10−4 H and a resistor with a resistance of R=6.28 Ω. Our goal is to find the Quality Factor (Q), a dimensionless parameter that describes how 'sharp' or 'selective' this resonance is.
The Master Equation
Quality Factor
The Quality Factor of a series resonant circuit is defined as the ratio of the resonant angular frequency times the inductance to the resistance. Mathematically, it is expressed as:
Since we are given the linear frequency f0 instead of the angular frequency ω0, we must remember the fundamental relationship ω0=2πf0. Substituting this into our master equation gives us a highly practical formula:
The Elegance of Numbers
Now, let's carefully substitute our known values into this equation. The problem explicitly instructs us to take π=3.14. This is a massive hint from the examiner!
Look closely at the numerator. If we multiply 2 by 3.14, we get exactly 6.28. This perfectly matches the resistance value in the denominator!
This allows for a beautiful, clean cancellation. The 6.28 in the numerator and the 6.28 in the denominator simply vanish, leaving us with a straightforward exponent calculation.
The Final Verdict
After the cancellation, we are left with:
Using the basic laws of exponents, we add the powers of 10: 7+(−4)=3.
Our final Quality Factor is 2000. A Q-factor this high indicates that the circuit is highly selective, meaning it has a very sharp resonance peak and loses very little energy per cycle compared to the energy it stores. It's a beautifully efficient resonator!