Feeds
Analysis & Design Software

Self-Resonant Frequency of Single-Layer Solenoid Coils

Author: R.J.Edwards G4FGQ © 18th November 2004

Coils have a distributed self-capacitance equivalent to a lumped capacitance connected between its ends. Consequently, all coils have a parallel resonant frequency. At resonance there's a very high impedance between the ends of the coil. A common application is use of a coil as a resonant RF choke.

For a single-layer solenoid the self-capacitance can be calculated from its dimensions. From the inductance, loss resistance and Q, the resonant frequency and impedance-vs-frequency response can be found.

A choke can be made from a length of close-wound, neatly-wound coaxial cable inserted in a coaxial line of the same type to minimise undesirable RF currents flowing on the outer surface of the coaxial line's outer conductor. It is necessary to calculate the approximate self-resonant frequency of the coil and the range of frequencies over which the choke impedance is high enough to be effective in a particular wideband application.

The impedance of a coaxial choke can be as high as several megohms at resonance, but in practice, an off-resonance impedance of 1000 ohms may be sufficient. Much depends on length of line in wavelengths and its terminating resistance.

Some Crude but Small Approximations
When a coil is connected between its connecting leads the small stray capacitance between the leads is placed across the coil and the coils' resonant frequency decreases. In the case of a coil in a long antenna wire or feedline the question arises over what lengths of lead is the capacitance between leads effectively in parallel with the coil? So what is the coil's resonant frequency?

As the length of the coil and the spacing between the leads increases the stray lead-to-lead capacitance decreases. On the other other hand it increases as the lead length increases but in a decreasing manner until it remains constant. Because capacitances of coil and leads are both distributed their resultant is not the arithmetic sum of the two - it is mathematically indeterminate.

The capacitance of a very short open-circuited lead IS calculable and increases in direct proportion to its length. But when leads are long only the length of lead immediately adjacent to the coil affects capacitance across the coil and it is necessary to guess the short length of the leads involved. At least, the guesswork allows the uncertainty to be estimated. Fortunately all is very uncritical. In the absence of any better guesses it is suggested lead length be set equal to coil length and results will probably be in the right ball-park.

Operating Notes

  • Number of Turns = Coil Length divided by Winding Pitch.
  • Winding pitch = Coil length divided by number of turns.
  • Winding Pitch = Wire Diameter + Twice Insulation Thickness + Twice air space.
  • For a coax choke, conductor diameter is diameter of coaxial outer conductor.

For a coax choke inserted in a long line, lead length is the initial short length of the line which has an appreciable affect on capacitance across the coil. The calculated resonant frequency with leads connected to the coil occurs when the line is cut and the resulting short leads are open circuited at their outer ends.

If instead of a neatly wound coil a 'jumble-wound' coil of the same mean diameter and number of turns is used then the self-resonant frequency and Q may fall by crudely 30 or 40 percent. More important, impedance vs frequency above resonance instead of smoothly decreasing is likely to vary erratically and the choke may not be effective at a few unpredictable frequencies above resonance. Ineffective may mean only that the choke impedance is less than 1000 ohms.

A minor advantage of a solenoid-wound coaxial choke over a ferrite-ring type is that the line impedance Zo remains constant throughout the system.

Random and Spurious Effects
At frequencies well above the fundamental resonant frequency there are further resonances between the coil and the coax line. Theoretically, at 3, 5 and 7 times the fundamental resonance, there will be other very high coil impedances which cause no problems. But at the even harmonics the impedance may fall to very low values which may render the choking action ineffective.

The actual frequencies at which even harmonics fall into an amateur band depend on line length and on coil location and are unpredictable. To be fairly sure of avoiding spurious resonances operating frequencies should be limited to twice the fundamental resonant frequency. On the other hand the chance of a spurious response falling in an amateur band is not very high and even if it does it may not have a serious effect anyway.

Choke Performance See Test Circuit
Performance is in terms of the insertion loss in decibels of RF power flowing along the wire, or coaxial outer conductor, due to insertion of the choke. The load impedance immediately on the choke is also indicated since this has a bearing on performance. Both figures are necessarily very approximate. They depend on line length in waves at the test frequency. Source impedance is 50 ohms.

Other Thoughts on the Subject
The only accurate numerical results of this program are the self-resonant frequency of the coil in free-space and the resonant frequency of the coil with open circuit leads connected, neither of which exists in practice because the leads, whatever their length, must be connected to the remainder of a more complicated circuit. Whatever is done affects distributed stray capacitances and mutual impedances and so also affect the coil's resonant frequency - the frequency at which the coil's impedance Z is a maximum.

The actual resonant impedance Z is very high but is seldom important. It is the bandwidth over which Z is more than some relatively low value which matters. It depends entirely on the choke's application, narrowband or wideband.

In the case of a choke made with coaxial line, the dimensions of which are very non-critical, it is the impedance at band edges which matters most. The effectiveness of which depends on the coil's location along the line, the line's length, and the standing waves which always exist on it.

A ferrite choke has sensibly zero transmission loss. But a large coaxial solenoid can have appreciable transmission loss due to its long coaxial length. Also a ferrite choke can have a fairly flat response and a wider usable bandwidth.

Circuit for Performance Test on Coaxial Choke

        50 ohms          L         R           Unbalanced Feedline
   o--------o---QQQQQQ------o-----------------------------o
                                           Length in Wavelengths    
                          CHOKE                                     
   o                                                                 Z
 Source            o-------------------o                 Adjustable  Z
 at Test Freq.                C                            Termination Z
                                                                      Z
                                                                      
   o Ground                                                     Ground o

Coil Q is calculated from R. Capacitor Q is assumed to be 2000. Line termination represents an uncertain low resistance ground connection.

Principal Computed Results

  • Self-capacitance of coil
  • Resonant frequency of isolated choke
  • Resonant frequency of choke when inserted in line
  • Magnitude of choke impedance vs test frequency
  • Insertion loss of choke in dB, vs line length in wavelengths, at test frequency

Run this Program from the Web or Download and Run it from Your Computer
This program is self-contained and ready to use. It does not require installation. Click this link SelfRes3 then click Open to run from the web or Save to save the program to your hard drive. If you save it to your hard drive, double-click the file name from Windows Explorer (Right-click Start then left-click Explore to start Windows Explorer) and it will run.


Search other ham radio sites with Ham Radio Search