Skip to main content

Calculation of the transmitter P - contour

P-contour Calculator for Power Amplifiers

Pi-network calculation based on the methodology of I. Goncharenko (DL2KQ).

To start the calculation, set your values for frequency F, source impedance R1, load impedance R2, unloaded coil Q-factor Qxx (assuming the unloaded Q of capacitors C1 and C2 is much higher than that of L, which is true for most capacitors), and your desired loaded Q-factor Qh. Then, click "Calculate".

For a tube amplifier operating in class AB with a small idle current, the source impedance R1 can be roughly estimated using the following formulas:
For the anode circuit, R1 ≈ Ea / (1.8 * Ia) (where Ea is the DC anode voltage and Ia is the maximum DC anode current) or R1 ≈ Ea² / (2.5 * P) (where P is the maximum effective output power).
For the input Pi-network of a grounded-grid PA, R2 ≈ 1/S (where S is the tube's transconductance).
The approximation of R1 is related to the conduction angle (i.e., idle current) and the type of tube, or more precisely, its minimum allowable instantaneous anode voltage.

Increasing the loaded Q-factor (Qh) of the Pi-network improves harmonic suppression and increases capacitor values (important for tubes with high output capacitance), but it lowers efficiency and increases reactive currents, imposing stricter requirements on component quality.

To evaluate the structural requirements for the Pi-network components, the calculator provides the effective current in the coil (to help select the wire cross-section) and in the capacitors (to help choose the contact quality, plate thickness, and dielectric). It also calculates the peak voltage (which capacitors must withstand with a safety margin) and the reactive power (in kVAr) for both capacitors.

For capacitors other than vacuum and air-variable types, the rule of thumb is: if the datasheet does not specify reactive power or allowable current at the operating frequency, the capacitor is likely not designed for high-power RF circuits and will burn out. Keep in mind that the voltage on the output capacitor can increase by 1.5 to 2 times depending on the antenna SWR and tuning accuracy. Leave a sufficient gap between the plates of C2 to prevent spark breakdown and plate welding when tuning the Pi-network at full power.

Input Parameters

Calculation Results

Actual Output Power (P)-
Power Losses in Coil-
Transmitter Efficiency-
Coil Inductance (L)-
Current in Coil-
Hot Capacitor (C1) Capacitance-
Cold Capacitor (C2) Capacitance-
Reactive Power in C1-
Reactive Power in C2-
Peak Voltage across C1-
Peak Voltage across C2-
Current through C1-
Current through C2-

Comments

Popular posts

Antenna calculation

Formulas for Dipole and Vertical Antennas Half-wave antenna in free space (15006 / F) cm Practical half-wave antenna (up to 30 MHz) (14274 / F) cm Half-wave antenna (50 to 144 MHz) (14030 / F) cm Half-wave antenna (above 144 MHz) (14233 / F) cm Quarter-wave antenna (7137 / F) cm Full-wave antenna length (30653 / F) cm Enter frequency (MHz): Calculate ...

Introduction to Electronics

Who Is This Tutorial For? This site is dedicated not only to beginner electronics enthusiasts but also to people who appreciate radio electronics as a fascinating field of science and technology, as well as a wonderful hobby. I hope that through my lessons, many will gain knowledge and find answers to questions that may have arisen while studying other sources of information regarding electronics. Since you have visited this page, you must already be interested in what is offered here. Perhaps this is exactly the tutorial you have been looking for, and I believe you will not be disappointed. For people who are already familiar with the basics of electronics and have practical skills, we plan to include interesting sections such as repairing household electronic equipment, communications (building receivers, transceivers, etc.), and microcontroller programming . The idea of creating a step-by-step tut...

What is Radio Electronics?

HOW DID SUCH A SCIENCE AS ELECTRONICS APPEAR? The purpose of this lesson is to give an idea of electronics as a science — a branch that, both in the past and today, fills its niche in almost all areas of the national economy, education, and technology. In this lesson, you will also get an idea of the structure of matter and electrically charged particles. We will also touch upon the structure of the atom, the concept of electricity, and the electrification of bodies. At the end of the lesson, there will be a small practical assignment. As the large encyclopedic dictionary tells us, ELECTRONICS is the science of the interaction of charged particles (electrons, ions) with electromagnetic fields and the methods of creating electronic devices and equipment (vacuum, gas-discharge, semiconductor), used mainly for the transmission, processing, and storage of information. Electronics as a science emerged in the early 20th century; initially, it was mainly vacuum electronics that...