Exactly what is Q, and how does it affect your circuits? Come along and see.
During the past few years, in the process of writing software for HAMCALC (a collection of programs of interest to Amateur Radio enthusiasts),(1) I kept hoping that I would eventually come across a clear, concise definition of coil Q, complete with a simple equation or two. That did not happen, so 1 decided a more aggressive search through the available literature was in order. I was able to compile definitions and a series of equations (see the Table of Equations) from the following sources (abbreviated titles shown are used throughout this discourse; the full titles are given in the Notes at the end of the article):
The main purpose of my investigation was not to introduce any new theory or interpretations, but to see if I could determine a logical sequence and correlation between existing, proven equations. My original published findings dealing with true Q(6) have been expanded and more equations added for inclusion in this paper.
To preserve the integrity of the equations, they are presented in the Table of Equations as they appear in the original reference sources-some in metric units, others in imperial units. This may be a bother when doing calculations manually, for which I apologize, but it presents no problem in the HAMCALC (version 50) computer programs where conversion is automatic.
C= added external capacitance required to resonate
Co = distributed capacitance, in pF
d = coil pitch circle diameter, in inches
fHz = operating frequency, in Hertz
fMHZ = operating frequency, in megahertz
fs = self-resonant frequency, in Hertz
Kp = 1.15 (proximity factor)
La = apparent inductance, in microheries
Lcm = coil length, in centimeters
Lgth = coil length, in inches, as a function of inductance
Lo = coil length, in inches, as a function of frequency and
Lµ = true inductance, in microheries
n = number of turns
Pf = 1 (assumed power factor)
π = 3.141593
Qa = apparent Q of coil
Qc = Q of coil due to self -capacitance
Qt = true Q of coil
Ra = resistance due to distributed capacitance, in ohms
Rac = RF resistance in ohms/cm.
Rc = coil pitch circle radius, in centimeters
Req = equivalent series resistance of coil
Ro = equivalent resistance of Cc, in ohms
Rsk = total skin-effect resistance, in ohms
Rt = true resistance, in ohms
Sd = winding pitch/conductor diameter ratio
Sw = winding pitch (center-to-center turn spacing), in inches
W = conductor diameter, in inches
Wmax = maximum conductor diameter, in inches
Wmin = minimum conductor diameter, in inches
The 1997ARRL Handbook(7) defines component Q as the ratioX/R, whereX is the reactance of the component and R is the sum of all resistances associated with energy losses in the component. Terman defines two separate values of coil Q:(8) true Qt and observed Q, True Qt (Eq 3) is a mathematical relationship between the radius and length of a "perfect" coil without losses, at a specific frequency when the turn spacing (Eq 6) is within the range of about 0.45 (Eq 8) to 0.70 (Eq 7) times the diameter of the conductor. Observed Q is the value observed by a Q meter.
Radiotron Handbook (page 451) refers to Terman's "observed Q" as "apparent Q". Apparent Qa (Eq 20), is less than true Qt because of the presence of distributed capacity (Eq 10, Eq 11) and resistive losses within the coil that affect the reading of a Q meter.
Terman observes(9) that with a given inductance and coil diameter, Q is maximum when the length/diameter ratio of the coil is in the order of 0.5:1. Actually, some iterative calculation using equation Eq 3 will show the maximum Q increases rapidly with L/d ratio, peaking in the L/d range of about 0.35:1 to 0.45A, then decreases gradually with L/d ratio (see Fig 1). This is consistent with Terman's popular rule of thumb, which probably includes a safety margin.
Fig 1 - Maximum Q of typical coils.
Terman states:(10) ". The presence of distributed capacity causes a partial resonance that modifies the apparent resistance and reactance of the coil as viewed from the terminals. The apparent series resistances La and Ra ... are related to the true resistance Rt and inductance Lp according to the equations . . ." (The equations(11) that follow Terman's statement are expressed in terms of the ratio [actual frequency] / [self-resonant frequency].
The Radiotron Handbook states:(12) "In all cases the self capacitance of a coil has an apparent effect on its resistance, inductance and Q, and at frequencies considerably below the self resonant frequency of the coil [are] ... Eqs 18, 19 and 20. These equations are expressed in terms of the ratio [self-capacitance of coil] / [external capacitance required to tune Lµ to resonance]. The equations (page 451) produce values identical to the Terman equations, which are not included in the Table of Equations.
In addition to distributed-capacitance losses, Terman describes four other factors(13) contributing to coil losses as:
At some sufficiently high frequency (Eq 12), inductors and capacitors become self-resonant. Just as in a tuned circuit, above that frequency, the capacitor will appear inductive and the inductor will appear capacitive.(16) Because of this, coils are not usually designed for operation above their selfresonant frequency, and any calculated or measured Q above the resonant frequency becomes meaningless in most practical applications.
True Qt, which has no losses, increases indefinitely with frequency. Apparent Qa increases with frequency, peaks at a point appreciably less than the self-resonant frequency and then, due to distributed-capacitance effect and resistive losses, decreases until it reaches zero at the coil's self-resonant frequency. These relationships are shown graphically in Fig 2.
Fig 2 - Values of Q for coil described in Fig 4: 34.7 pH, 27 turns of #14 AWG at 8 turns per inch on a 3-inch diameter form. The coil is 3.375 inches long.
This is mostly ajudgement call based on experience. Because there is little in the literature for guidance, and what little mention there is apparently refers either to apparent Qa or to measurements made by a Q meter under unspecified conditions affecting the interpretation of the meter reading. As a rule, a high apparent Qa is required for narrow bandwidth, minimum bandwidth noise and maximum efficiency.
A useful feature of the HAMCALC Q Calculator program is that as soon as the basic requirements (conductor diameter, inductance and frequency) are entered, it immediately computes and displays the approximate maximum true Q for those factors.
The tricky part in designing a coil with a specific Qt is to arrive at a length and diameter where the length Lgth as a function of inductance (Eq 4) is equal to the length Lo as a function of frequency and true Qt (Eq 5). To design a coil with a specific true Qt, using the equations here, determine five known factors:
Proceed with the design calculations as follows:
Because of the iterative nature of the calculations, this can be a tedious manual operation. To design a coil with a specific apparent Qt using a computer, decide four known factors:
With HAMCALC loaded in your computer, start the Coil Q Calculator program, and proceed as follows:
Fig 3 - Inerim results from the coil Q calculator show possible coils for the specified conductor diameter, inductance and frequency.
Fig 4 - After selecting a coil diameter of 3.0000", coil Q calculator dislplays the various properties of that coil.
The HAMCALC Coil Equation Calculator may also be found useful in preliminary design and analysis of new or existing single-layer air-core coils. Given only a few of any known properties of a coil, it computes most of the other commonly sought properties, including true Qt and apparent Qa.
Nothing very new is presented in this paper, but I hope it may make life a little easier for the coil designer by presenting most of the pertinent equations in one place. Anyone interested in surfing the equations by computer can obtain a free program to do just that by e-mailing a request for QSOLVE.BAS to email@example.com.(17)
Eq 1: 1997 ARRL Handbook, page 6.22 equation 44.
Eq 2: 1997 ARRL Handbook, page 6.22 equation 45.
Eq 3: Radiotron Handbook, page 464 equation F.
Eq 4: Derived from Eq 1 or Eq 2.
Eq 5: Derived from Eq 3 and converted to inches.
Eq 6: Ratio of coil length, in inches, to number of turns.
Eq 7: Eq 8: Radiotron Handbook, page 463 (A), page 464 (B) (G), page 465 (G) (a), page 465 (H) (d).
Eq 9: Ratio of coil winding pitch to conductor diameter.
Eq 10: Electronic Equations Handbook, page 6 equation 1-38.
Eq 11: Eq 10 with cosh function re-phrased to suit calculation by computer.
Eq 12-13: Derived from the ARRL Handbook, page 6.35 equations 89 to 92.
Eq 14: Terman Handbook, page 34 equation 5.
Eq 15: Terman Handbook, page 35 equation 6.
Eq 16: Total conductor-resistance equation Rac x conductor length, in cm.
Eq 17: Total resistance.
Eq 18-20: Radiotron Handbook, page 451 (1).
The interpretation of readings displayed by Q meters is beyond the scope of this article. According to the manual I have for one of these instruments, there is a lot more to measuring coil Q than merely attaching a couple of test leads, pushing a button and getting an instant result. If anyone wants an article about how to read a Q meter, it won't be written by me. I don't even understand the manual!