The resonant frequency of an RLC circuit is the frequency at which the inductive reactance (\(X_L\)) and capacitive reactance (\(X_C\)) cancel each other out, resulting in the circuit's impedance being purely resistive (i.e., equal to the resistance \(R\) of the circuit). At resonance, the circuit oscillates at its natural frequency with minimal energy loss, and the current is at its maximum for a given applied voltage.
### Formula for Resonant Frequency
The resonant frequency (\(f_0\)) for an RLC circuit is calculated using the following formula:
\[
f_0 = \frac{1}{2\pi\sqrt{LC}}
\]
where:
- \(L\) is the inductance in henrys (H),
- \(C\) is the capacitance in farads (F),
- \(f_0\) is the resonant frequency in hertz (Hz).
This formula applies to both series and parallel RLC circuits, as resonance is defined by the same condition in both types of circuits.
### Explanation of the Formula
1. **Inductive Reactance (\(X_L\)):**
- The inductive reactance of an inductor increases with frequency, and it is given by:
\[
X_L = 2\pi f L
\]
- Here, \(f\) is the frequency and \(L\) is the inductance. Inductive reactance causes the current to lag behind the voltage.
2. **Capacitive Reactance (\(X_C\)):**
- The capacitive reactance of a capacitor decreases with frequency, and it is given by:
\[
X_C = \frac{1}{2\pi f C}
\]
- Here, \(C\) is the capacitance, and capacitive reactance causes the current to lead the voltage.
3. **At Resonance:**
- At the resonant frequency \(f_0\), the inductive reactance \(X_L\) and the capacitive reactance \(X_C\) are equal in magnitude but opposite in phase. Thus, they cancel each other out, leading to a net reactance of zero:
\[
X_L = X_C \quad \Rightarrow \quad 2\pi f_0 L = \frac{1}{2\pi f_0 C}
\]
- Solving for \(f_0\), we get the resonant frequency:
\[
f_0 = \frac{1}{2\pi \sqrt{LC}}
\]
### Steps to Calculate Resonant Frequency
1. **Identify the inductance (L)** of the inductor in the circuit. This should be in henrys (H).
2. **Identify the capacitance (C)** of the capacitor in the circuit. This should be in farads (F).
3. **Substitute** the values of \(L\) and \(C\) into the formula \(f_0 = \frac{1}{2\pi\sqrt{LC}}\).
4. **Solve for \(f_0\)** to find the resonant frequency in hertz (Hz).
### Example
Let’s calculate the resonant frequency for a circuit with:
- \(L = 10 \, \text{mH} = 10 \times 10^{-3} \, \text{H}\),
- \(C = 100 \, \mu\text{F} = 100 \times 10^{-6} \, \text{F}\).
Using the formula:
\[
f_0 = \frac{1}{2\pi \sqrt{(10 \times 10^{-3})(100 \times 10^{-6})}}
\]
First, calculate the product inside the square root:
\[
L \times C = (10 \times 10^{-3})(100 \times 10^{-6}) = 10^{-6}
\]
Now take the square root:
\[
\sqrt{L \times C} = \sqrt{10^{-6}} = 10^{-3}
\]
Now, substitute into the formula:
\[
f_0 = \frac{1}{2\pi \times 10^{-3}} = \frac{1}{0.00628} \approx 159.15 \, \text{Hz}
\]
So, the resonant frequency \(f_0\) is approximately 159.15 Hz.
### Importance of Resonance in RLC Circuits
At resonance:
- **Maximum current** flows through a series RLC circuit because the impedance is minimized to just the resistance \(R\).
- In a **parallel RLC circuit**, resonance causes the total current drawn from the source to be minimized because the circuit behaves like an open circuit at resonance.
- Resonance is widely used in applications like radio tuners, filters, and oscillators, where selecting or rejecting specific frequencies is essential.
By using the simple formula \(f_0 = \frac{1}{2\pi\sqrt{LC}}\), you can easily determine the resonant frequency of an RLC circuit.