Active Components

Clapp Oscillator

An engineer builds a 50 MHz Colpitts oscillator for a radio transmitter. When they turn it on, the frequency is perfect. However, as the amplifier transistor heats up, its internal junction capacitance expands. Because this parasitic capacitance is directly parallel to the resonant tank, the output frequency slowly drifts down to 48 MHz, rendering the radio useless. To solve this thermal drift, the engineer upgrades to a Clapp oscillator topology. They insert a third capacitor (C3) in series with the main inductor. By making C3 much smaller than the divider capacitors, the mathematical series capacitance forces C3 to dominate the resonant frequency equation. The tank is now decoupled from the transistor. Even as the transistor heats up and its internal capacitance wildly fluctuates, the oscillator remains rock-solid at exactly 50 MHz. The Clapp topology is the ultimate refinement of discrete LC stability.
Category: Active Components
Topology: Colpitts + Series Inductor Capacitor
Primary Benefit: Transistor capacitance isolation

Oscillator Topology Comparison

TopologyFeedback NetworkTuning ElementFrequency Stability
HartleyTapped Inductor (L1, L2)Parallel CapacitorPoor (Mutual inductance issues)
ColpittsCapacitive Divider (C1, C2)Parallel InductorModerate (Vulnerable to transistor drift)
ClappCapacitive Divider (C1, C2)Series Capacitor (C3)Excellent (Isolated from transistor)
PierceCrystal ResonatorCrystal CutUltimate (ppm precision)
Clapp Resonant Frequency:
f = 1 / [ 2π · √(L · Ceq) ]
Where the equivalent capacitance Ceq is:
1 / Ceq = (1 / C1) + (1 / C2) + (1 / C3)

The Stability Math:
If C3 is intentionally chosen to be much smaller than C1 and C2 (e.g., C3 = 10pF, C1=1000pF, C2=1000pF), then 1/C3 becomes the massive dominating term in the equation. Ceq becomes almost entirely equal to C3. Because the transistor's parasitic capacitance only fluctuates in parallel with the large C1 and C2, its impact on the total Ceq (and therefore the frequency) is mathematically marginalized.
Common Questions

Frequently Asked Questions

How do you tune a Clapp oscillator?

Unlike a Colpitts oscillator where you typically have to physically squeeze or stretch the inductor coil to change the frequency, the Clapp oscillator is tuned using the series capacitor (C3). By replacing C3 with a variable capacitor (or a voltage-controlled varactor diode), you can smoothly tune the frequency over a wide range without altering the feedback divider ratio established by C1 and C2.

What causes a Clapp oscillator to fail?

Lack of loop gain. The series addition of C3 raises the total impedance of the resonant tank branch. If you make C3 too small (in an attempt to gain maximum stability and wide tuning range), the tank impedance becomes so high that the transistor cannot push enough current through it to sustain oscillation. The circuit will simply sit there, completely dead, unable to meet the Barkhausen start-up criterion.

Is the Clapp oscillator still used today?

In modern high-frequency microwave design (Wi-Fi, 5G), discrete LC oscillators are obsolete due to poor phase noise. They have been replaced by Phase-Locked Loops (PLLs) driven by quartz crystals. However, the Clapp topology is still heavily used in amateur radio (VFOs), low-frequency RF test equipment, and specialized sensors where a wide, continuous tuning range is required without complex digital synthesis.

Active Design

Oscillator Stability Calculator

Input your desired frequency and the parasitic capacitance range of your transistor. Compare the frequency drift of a standard Colpitts against a Clapp topology and calculate the exact C3 value required for thermal immunity.

Calculate Drift Immunity