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Published: 30 March 2015

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Flat PCB coils are most often used in the VHF and UHF bands to reduce the size of the device. Usually they are produced with round, square or meander form of turns, although it can be in the form of a polygon. With the advent technology of multilayer PCB the multilayer coil appears. The use of a magnetic core is ineffective because such a core is far away from the turns of the coil and can change its inductance by 3  5 %, which in most cases is not enough. Therefore, printed inductors are used in most cases when the adjustment is not required and the value of the inductance units does not exceed microhenry. Qfactor of PCB inductors is generally lower then Qfactor of the inductors having a coil of wire and less than that of the cylindrical microstrip coils. The self capacitance of the printed inductors depends on the width of the spiral turns, the gap between them and the PCB material and can reach 3 to 5 pF, which is pretty high at such frequencies. All I have said is not in favor of flat PCB coils, however, the compact design along with the use of SMD components often plays a decisive role in use such inductors.
On our site you can use the online calculator to calculate the coils on PCB.
To compute inductance of PCB inductors we can use three pretty accurate methods.
1.The first approximation is based on a modification of an expression developed by H.A.Wheeler for the planar spiral inductors:
The coefficients K_{1} and K_{2} are layout dependent and are shown in following table:
2.The second is a monomial expression derived from fitting to a large database of inductors (and the exact inductance values):
where g = s  W gap between turns and the coefficients β and α_{i} are layout dependent and given in the following table:
This formula is used in Coil32 for square PCB coil calculation.
3.The third is derived from electromagnetic principles by approximating the sides of the spirals as currentsheets:
where
 L inductance (nH);
 D  outer diameter of coil (mm);
 d  inner diameter of coil (mm);
 N  number of turns;
 D_{avg}  average diameter of coil (mm);
 φ  fill factor;
 ci  factors from Table III (layuot depending):
For PCB inductor with round turns Coil32 uses the third method. The rearranged formula [3] is shown as:Although the accuracy of this expression worsens as the ratio s/W becomes large, it exhibits a maximum error of 8% for s ≈ 3W. Note that typical practical integrated spiral inductors are built with w ≤ s. For highest Qfactor the optimum ratio d/D = 0.4 for circle coil and optimum d/D = 0.362 for square coil. The program automatically set inner diameter value for this ratio. In the calculation, we define the outer diameter of the coil and its layout. If the result of the calculation obtained unacceptable sizes of printed trace, the outer diameter we can modify and recalculate the coil again.
In all expressions D_{avg} factor is average diameter of the coil and φ is the filling factor that represents how hollow the inductor is. Theese factors are defined as:
 D_{avg}  average diameter of coil;
 φ  fill factor;
 D  outer diameter of coil;
 d  inner diameter of coil;
All dimentions in meter, inductance in henry. All three expressions are accurate, with typical errors of 2–3%, and very simple, and are therefore excellent candidates for use in design and synthesis PCB inductors.
Inductor as a straight microstrip calculates by the following expression:
 L  inductance (μH)
 l trace length (mm)
 b  trace width (mm)
Such inductive elements are often used in filters UHF band. Because of what the selfcapacitance of such inductive element is quite large, it is necessary to keep in mind that the more correct to represent it in the form of a segment of a transmission line with distributed parameters. However, for approximate calculations, this model is quite acceptable if this element works at frequencies much lower the selfresonance.
Plugin meandr_PCB allows to calculate PCB inductors with meander layout of turns.
References:
 Simple Accurate Expressions for Planar Spiral Inductances  Mohan, S.S. ; Dept. of Electr. Eng., Stanford Univ., CA, USA ; del Mar Hershenson, M. ; Boyd, S.P. ; Lee, T.H. 1999
 Lumped Elements for RF and Microwave Circuits  Inder Bahl 2003