In An AC Current Generator, Part 1, I talked about the overall principle in creating an AC current generator. Today I am going to start to describe how to create a transformer, specifically to generate 10 amps AC. It is rather detailed and lengthy, so I am going to have to split it into multiple parts. The process is similar for any desired output current.

When testing, a 10 amp AC current is fed into the module being tested (DUT) and the current is measured across a 25 mÎ© shunt internal to the DUT. The arrangement can be represented by the circuit in Figure 2-1.

**Figure 2-1**

The output current from the power amplifier has three components of three different phases. I_{L} is the current through the inductive component; I_{R} is the current through the reflected resistive component (from the secondary); and I_{C} is the current through the capacitance of the circuit. An additional capacitor can be added to the parasitic already present to cancel the current required by the inductive component, reducing the current drive requirements of the amplifier.

The internal resistance of the secondary R_{i} is made up of wire resistance, plus the transferred impedance of the primary, plus the resistance of the measurement shunt and the transferred impedance from the secondary of the current measuring transformer. R_{L} is the shunt in our DUT.

**Step 1: Establish constants**

In order to design the transformer, we must introduce values from the actual circuitry that we are going to use. For this example we decided to generate an output current of 10 amps AC. The load R_{L} is 25 mÎ© (the shunt internal to the product), and the wiring resistance of the secondary, Ri is assumed to be 25 mÎ© as well.

The Bicron B5303 current transformer (BICRON_Current_Sensors) has a current turns ratio of 5,000 and a wire resistance of 207 ohms. The output is connected in series with a 10 ohm resistor in its secondary (internal to the measurement device). The reflected impedance is 217/5000^{2} = 9 ÎĽ Î© so this should not pose a problem and is included in the nominal 25 mÎ©.

A transformer core must be selected. We had several spare toroidal transformers, which we disassembled. The measurements of the transformer core selected were as follows:

- Crossâ€“sectional height H = 2.15 cm

Cross-section width W = 1.60 cm

Inner diameter D = 3.93 cm

Prior to the other calculations the inductance per turn L_{T} must also be known. This can be calculated from the magnetic constants if the core data is available using the following formula:

- Inductance of the winding, L (in Henry) = (1.256*S*N

^{2}* ÎĽ

_{e}*10

^{-8})/C

_{m}â€¦â€¦â€¦(1)

Where S is the core cross section in square cm, C_{m} is the mean circumference of the toroid (2* Î *(outside diameter-inside diameter)/2), and N is the total number of turns. ÎĽ _{e} is the effective permeability of the material. In a toroid this is essentially the permeability of the material. Once L has been calculated from the above formula, L_{T} can be simply calculated as follows:

- L

_{T}= L/ N

^{2}â€¦â€¦.(2)

However, if you are like us, you donâ€™t have those details, so alternatively it can be measured with an LCR bridge. Winding 5 turns through the core and measuring the inductance gave 40.7 ÎĽ H. Using (2) above L_{T} is calculated as 40.7/52 = 1.63 ÎĽ H/turn^{2} .

**Step 2: Primary turns**

Just to be sure that our numbers will work I remind you that the maximum allowable flux density before saturation of an iron core is 12,000 to 15,000 gauss. 8,000 to 10,000 gauss is a safe value. Iron cores can be used up to a frequency of 400 Hz. For higher frequencies a ferrite core must be used where the flux density must be reduced to no more than 2,500 to 3,000 gauss to prevent saturation of the core. So there!

Magnetic theory predicts the following relationship for the primary of the transformer:

- E=4.44*f*N

_{P}*S*B*10

^{-8}â€¦â€¦.(3)

Where E is the RMS voltage, f is the frequency, N_{P} is the number of turns on the primary, S is the cross sectional area of the core, and B is the flux density in the core (in gauss).

We can re-arrange this to find the number of turns:

- N

_{P}= (E*10

^{8})/(4.44*f*S*B) â€¦â€¦.(4)

In our setup E=14Vrms. This is derived from the supplies being +/-24V. Allowing for 4V â€śheadroomâ€ť for the power amplifier, this gives V_{pp} of 40V.

- V

_{rms}= V

_{pp}/(2*1.414)=E â€¦â€¦.(5)

The frequency, f, is nominally 60Hz.

The cross sectional area, S is equal to H*W=2.15*1.60=3.44 cm^{2}

The constant B is our flux density of 8,000 gauss.

Substituting these values

- N

_{P}= (14*10

^{8})/(4.44*60*3.44*8000) â‰…190 turns â€¦â€¦.(6)

This is the number of turns required to maintain the core below saturation at the maximum input voltage.

This number of coils can be quite difficult to wind and you can see how to do it in Hint No 3 in my blog, â€śTop 17 Helpful Hints for Constructing Electronic Systems.â€ť

**Step 3: Secondary turns**

The next step is to calculate the number of turns on the secondary, N_{s} . As can be seen from Figure 2-1 and based on Ohmâ€™s Law:

- Vout = Iout*(RL+Ri) â€¦â€¦.(7)

Since we have chosen the output to be 10Amps and RL=25 mÎ© and Ri=25 mÎ©, Vout=10*0.05=0.5Vac.

The turns ratio is the proportion of the input voltage to the output voltage n= E/Vout=14/0.5 = 28.

Therefore the number of turns on the secondary N_{s} :

- N

_{s}= N

_{p}/n = 190/28 = 7.

We have calculated the primary and secondary turns, but we still have to figure out what gauge of wire to use on the primary and secondary, to say nothing of reflected impedances. I will leave you on tenterhooks till Part 3.

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Coli winding design could be a crucial in terms of power efficiency. Coil winding machine could be used for mass production in manufacture and decide the transformer durability depending on primary winding and secondary winding. A few engineers might check actual transformer design.Â Â

Thanks for the series, @Aubrey, and for pointing us to your top 17 helpful hints post.

Toroid transformers perform great as magnetic flux can stay more confined than in E section transformers, that makes them attractive in many applications. But winding a high number of turns into a toroid transformer can be time consuming and laborious.

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