@joulupukki and @mountainhick
You don't necessarily need an app. You can use Merlin's method of estimating the source resistance and then use his chart to estimate the B+ and the ripple current based on the source/load ratio.
I'll walk through simulating it in LTspice first using the specs for the 50VA 05TC300 from their datasheet. I'm not going to do a complete tutorial on LTspice. I'm just going to go through a few models to show how we can simplify this down to Merlin's method.
Hopefully @andrewRneumann will check this for accuracy.
View attachment 1027717
The first thing we need to do is calculate is the turns ratio. Antek gives an input voltage of 120 Vrms and an unloaded output voltage of 310 Vrms.
Vpri = 120
Vsec = 310
Turns ratio = Vpri / Vsec
120 / 310 = 0.38709...
The impedance/inductance ratio is the turns ratio squared.
Inductance ratio = (Vpri/Vsec)^2
0.38709... ^ 2 = 0.14984...
In LTspice we'll create 4 inductors with mutual inductive coupling to simulate the two primary coils and the two secondary coils. We don't know what the actual inductance values are for those coils, and we don't really need to know for a simple model. We can just use an arbitrary high value of 100 henrys for the primary coil, and calculate a value for the secondary coils using the inductance ratio.
View attachment 1027734
Using the inductance ratio, we calculate a value for the secondaries:
100 / 0.14984... = 667.36111...
We create two 100H inductors, L1 & L2, to simulate the primaries, and two 667.311H inductors, L3 & L4, to simulate the secondaries. We give these mutual inductance with the K statement (K1 L1 L2 L3 L4 1). We also need to add the DC resistance for each coil. So we create resistors in series with the inductors using the values from the Antek datasheet (note that in LTspice you could simply add the series resistances to the inductor properties instead of creating separate resistors).
We add a voltage source for the 120Vrms 60Hz mains input. In LTspice this needs to be Vpeak, not Vrms.
Vpeak = Vrms x sqrt2
120 x 1.41421... = 169.70562...
Lastly, we need a load to simulate. Going by the datasheet example, 295Vrms output with a 60mA load. Using Ohm's law:
295 / .06 = 4916.66666...
Adding a 4916.67 ohm resistor for the load, and running a simulation (0ms to 100ms = 6 cycles):
View attachment 1027762
Vrms: 298V
Irms: 60.609mA
The voltage is off by about 1% compared to the datasheet, most likely because we are not modeling any losses.
Since we're probably going to be using the primaries and the secondaries in parallel, we don't really need to model all of the coils, so we can simplify the model by combining them. The turns ratio doesn't change. We just need to divide the series resistances in half.
View attachment 1027770
Running the simulation we get the exact same results:
View attachment 1027771
Vrms: 298V
Irms: 60.609mA
Now, moving on to Merlin's method found here:
In that article, he describes how to calculate the source resistance of a transformer as follows.
The source resistance is equal to the resistance of the secondary coil, plus the resistance of the primary coil when 'reflected' to the secondary:
Rs = Rsec + Rpri/(Vpri/Vsec)^2
Where:
Rsec = measured resistance of the secondary winding.
Rpri = measured resistance of the primary winding.
Vpri = RMS primary voltage (e.g., mains voltage).
Vsec = RMS secondary voltage measured with no load.
We already did part of this calculation, which is finding the impedance/inductance ratio.
120V / 310V = 0.38709...
0.38709... ^ 2 = 0.14984...
The DCR of each primary is 22 ohms. In parallel that's 11 ohms. We take the combined resistance of the primary and divide it by the impedance ratio, which gives us the reflected impedance of the primary.
11 ohms / 0.14984... = 73.40972... ohms
Now we add that value in series to the resistance of the secondary. Since each secondary coil is 235 ohms, that's a parallel resistance of 117.5 ohms.
117.5 ohms + 73.40972 ohms = 190.90972 ohms
We can get rid of the inductors in our model, and simply use a series resistance of 190.91 with a voltage source. The voltage source will be the unloaded secondary voltage. In LTspice, this needs to be Vpeak (310 x sqrt2).
View attachment 1027795
Running the simulation we get practically the same result, accounting for rounding errors.
View attachment 1027800
Vrms: 298.01V
Irms: 60.612mA
So far, all we've done is simulate an AC load to show how we can model just a transformer. That's all I have time for at the moment. I'll post an update with rectification and filtering, and we'll compare it to Merlin's source/load ratio chart and calculations.
+1 to this question. My best guess is that it's the average DC current drawn by the amp as described by The Valve Wizard but would you also include the heater lines in that calculation or ignore them since they are not the main secondary lines we're talking about?@Phrygian77
In your example, you hypothesize a 60 ma load. How specifically do you come up with that total in a real world case? The spec sheet combined max current ratings for the tube plates and screens? Or any derating?
+1 to this question. My best guess is that it's the average DC current drawn by the amp as described by The Valve Wizard but would you also include the heater lines in that calculation or ignore them since they are not the main secondary lines we're talking about?
Edit: my best guess is that we ignore the heater part of the circuit/transformer since I don't see any of that in the calculations so far. Seems like for heaters, as long as the transformer provides enough current (and the right voltage) for the tubes you're using, should be good to go.
@Phrygian77
In your example, you hypothesize a 60 ma load. How specifically do you come up with that total in a real world case? The spec sheet combined max current ratings for the tube plates and screens? Or any derating?
Thanks, Tail between legs.I was using the AC load reference in the Antek datasheet for the 05TC300. I thought that I said that in my post. In fact, I said that the model was off by 1% compared to the datasheet. Look again at the Antek datasheet (where I circled it in red in my post). It shows at 0A (no load) 310 VAC RMS output, and right below that in the table, 295 VAC RMS output at 0.06A. My point was to show that the estimated source resistance and output was close to real word (or at least as specified by Antek).
60 x .00004 x 9889.92 ≈ 24
This number just represents the amount of filtering relative to the load, and as you can see from Merlin's graph, there's not a lot of difference here between 2 and 1000.
310 x 1.23 = 381.3
Our estimated B+ is approximately 381 Vdc. That's a pretty big drop from 426.26 Vdc, which is due in part to the source resistance. To quote Merlin ...
Maybe this would cause us to re-think the amplifier design, or maybe we would consider it OK.
For our example, the ripple current will roughly 1.9 times the load current.
38.55 mA x 1.9 ≈ 73.25 mA
@andrewRneumann I almost didn't post that because, as I got into it, I realized there maybe questions that I couldn't answer about it. Merlin's graphical method seems to give slightly lower B+ numbers than I get out of LTspice. I'm wondering now how Merlin came up with them to begin with.
Does Merlin live GB? Possibly 50Hz mains make some of the difference to yours when discharge time is up to 20% longer?
f*C*Rl should account for that. I've been trying to think of a better why to describe that. On the graphs, it essentially represents represents the total AC load.
I feel like the guy at the back of the class who's hoping the professor doesn't call on to answer questions.Cool thread, you guys. I feel like the freshman looking for his pre-calc 101 class stumbling into a graduate seminar on Real and Complex Analysis. But the drawings on the board are beautiful...![]()