Where Does the Formula for L_0 in Audio Output Transformers Come From?

AI Thread Summary
The discussion centers on understanding the formula for L_0 in audio output transformers, specifically its derivation and the significance of the magnetic path length (l). Participants clarify that the formula incorporates the conversion from meters to inches, resulting in the constant 3.2E-8. The magnetic path length is identified as 4.5 inches, representing the mean flux path length. Additionally, there is a debate about the correct formulation of inductance, with some arguing that the inductance should be expressed per unit length rather than as a total inductance. The conversation also touches on the differences in equivalent circuit representations from various sources.
yungman
Messages
5,741
Reaction score
294
I am reading audio output transformers. This is a paragraph from RDH4 and I don't understand where the formula of L_0\; come from. Please see attachment.
 

Attachments

  • Tr2.PNG
    Tr2.PNG
    20.4 KB · Views: 509
Engineering news on Phys.org
It looks like it's just L = \mu \mu_0 N^2 A/l where \mu_0 \simeq 1.26 E-6 H/m is folded in with the conversion from meters to inches to give the combined constant of 3.2E-8.
 
Last edited:
uart said:
It looks like it's just L = \mu \mu_0 N^2 A/l where \mu_0 \simeq 1.26 E-6 is folded in with the conversion from meters to inches to give the combined constant of 3.2E-8.
Thanks for the reply. What is the magnetic path l?

L_0=\frac {3.2A\mu N^2}{10^8\times l}

Also where is 3.2EE2 come from. \mu_0\;=1.256EE-6 won't get 3.2EE2.

Thanks

Alsn
 
Last edited:
yungman said:
Thanks for the reply. What is the magnetic path l?

L_0=\frac {3.2A\mu N^2}{10^8\times l}

Also where is 3.2EE2 come from. \mu_0\;=1.256EE-6 won't get 3.2EE2.

Thanks

Alsn

No, the geometric factor A/l just has units of length. In SI units you use m^2 and m to give A/l in meters. Then of course you use \mu_0 in H/m (1.26E-6 H/m).

If however you use inches for A/l then you'll need \mu_0 in H/in, so approx divided by 39.4 to give 3.2E-8
 
Thanks, so it's just going from meter to inches.

So what is the path length [itesx]l[/itex]? It was given 4.5 inches, where is this come from? Is this the length of the coil?
 
yungman said:
Thanks, so it's just going from meter to inches.

So what is the path length [itesx]l[/itex]? It was given 4.5 inches, where is this come from? Is this the length of the coil?

Yeah, it's the mean flux path length. :smile:
 
Thanks Uart, you are of big help.
 
Actually I have another question:

We know for solenoid, B=\mu_0\mu n I\;\hbox{ where n is number of turns per unit length.}

So L=\mu_0\mu n^2 A \;\hbox{ where A is the cross section area of the solenoid.}

The equation in the article, N is the total number of turns in the given length. so:

n=\frac N l\;\Rightarrow\; n^2=\frac {N^2}{l^2}

With that L_0\; should be:

L_0= \frac {3.2A \mu_0\mu}{10^8}\frac{N^2}{l^2}\;\hbox{ instead of }\;L_0= \frac {3.2A \mu_0\mu}{10^8}\frac{N^2}{l}
 
yungman said:
With that L_0\; should be:

L_0= \frac {3.2A \mu_0\mu}{10^8}\frac{N^2}{l^2}\;\hbox{ instead of }\;L_0= \frac {3.2A \mu_0\mu}{10^8}\frac{N^2}{l}

No, the equation you post for the solenoid is not for the total inductance, it is for the inductance per unit length. It should read :

\frac{L}{l}=\mu_0\mu n^2 A
 
  • #10
uart said:
No, the equation you post for the solenoid is not for the total inductance, it is for the inductance per unit length. It should read :

\frac{L}{l}=\mu_0\mu n^2 A

Thanks, do you go to sleep? I put in my sleeping in between these posts and you're still here!

So basically the total inductance is take the inductance per unit length times the length:

L_0= \frac {3.2A \mu_0\mu}{10^8}\frac{N^2}{l^2} \times l \Rightarrow \; L_0= \frac {3.2A \mu_0\mu}{10^8}\frac{N^2}{l}
 
  • #11
I have a different question, below is the equivalent circuit from the book: The first image is the part in question about the input impedance. The middle picture is the equivalent circuit at different frequency from the book.

The last picture on the right is my equivalent circuit. The top is the equivalent circuit of the real transformer.
(1) is the equivalent circuit refer to the primary.
(2) is the low frequency equivalent.
(3) is the equation of RA using my equivalent circuit which is different from the book in the first image.
(4) is the high frequency equivalent.

As you can see, the way I draw the equivalent circuit is different from the book, I don't think I can agree with the derivation of the book in the first image on the left. Even the equivalent circuit from the book Handbook of Transformer Design and Application by Flanagan and Wikipedia agree with me as in (1) of my drawing:

http://en.wikipedia.org/wiki/Transformer
 

Attachments

  • Freq limit.PNG
    Freq limit.PNG
    13.8 KB · Views: 466
  • TrEq2.PNG
    TrEq2.PNG
    16.2 KB · Views: 438
  • Equiv1L.png
    Equiv1L.png
    48.2 KB · Views: 478
Last edited:
  • #12
Anyone?
 
Back
Top