Reactance vs Frequency
How to Use
- Inductance L slider — set the inductor value (0.1 µH to 100 mH, log scale).
- Capacitance C slider — set the capacitor value (1 nF to 100 µF, log scale).
- Frequency f slider — move the cursor line to read XL and XC at any frequency.
- The Log Scale button toggles between logarithmic and linear axis display.
What to Observe
- The red curve (XL = 2πfL) rises linearly on the log-log plot — inductors oppose higher frequencies more.
- The blue curve (XC = 1/2πfC) falls linearly — capacitors oppose lower frequencies more.
- The two curves cross at f₀ (the resonant frequency) — the purple dot marks this point.
- At f₀, XL = XC and the reactances exactly cancel in a series or parallel LC circuit.
- The resonant frequency f₀ depends on both L and C: changing either moves the crossover left or right.
- At very low frequencies: XC → ∞ (capacitor = open), XL → 0 (inductor = short).
- At very high frequencies: XL → ∞ (inductor = open), XC → 0 (capacitor = short).
Key Equations
\[X_L = \omega L = 2\pi f L \quad \text{(increases with frequency)}\]
\[X_C = \frac{1}{\omega C} = \frac{1}{2\pi f C} \quad \text{(decreases with frequency)}\]
\[f_0 = \frac{1}{2\pi\sqrt{LC}} \quad \text{(resonant frequency: } X_L = X_C\text{)}\]
| Frequency | Inductor | Capacitor |
|---|---|---|
| DC (f=0) | Short circuit (XL=0) | Open circuit (XC=∞) |
| f₀ | XL = XC | XL = XC |
| High f | Open circuit (XL→∞) | Short circuit (XC→0) |
Key Concepts
- Inductive reactance XL: Opposition to current by an inductor; proportional to frequency
- Capacitive reactance XC: Opposition to current by a capacitor; inversely proportional to frequency
- Resonant frequency f₀: Frequency at which XL = XC; reactances cancel
- Log-log plot: Both reactance curves appear as straight lines with slopes +1 (XL) and −1 (XC)