Transformer efficiency at low (and high) frequencies

AI Thread Summary
Transformer efficiency decreases at low frequencies primarily due to the effects of mutual induction and back EMF, which limit current flow. As frequency decreases, the circuit behaves more like DC, leading to reduced voltage and increased risk of excessive current that can damage equipment. Hysteresis losses in the transformer core, which are minimal at 60 Hz, become more pronounced at higher frequencies. Laminated steel cores are commonly used to minimize these losses, while ferrite materials are preferred for very high frequencies. Understanding these factors is crucial for optimizing transformer performance across different frequency ranges.
v0id
Messages
42
Reaction score
0
Hello,

I've been thinking about why (elementary) transformer efficiency drops drastically at very low frequencies. I know hysteresis effects play a major role in reducing efficiency at high frequencies, but why low? I realize that as we reduce the frequency of the emf, we're making the circuit "more and more DC", but a freqency still exists, no? The transformer that I'm talking about is a simple two-solenoids-magnetically-linked-by-a-ferromagnetic-core single phase one (home-made). Any help would be greatly appreciated.
 
Engineering news on Phys.org
>I realize that as we reduce the frequency of the emf, we're making the circuit "more and more DC"...

You've basically answered your own question.
The phenomenon of mutual induction (a.k.a. back EMF) between conductors in a transformer (or motor) winding is what limits the current. A very large utility distribution transformer will have 735 Kv on a primary winding of only a few ohms resistance. (0 ohms if they could make it). The equipment is designed to work efficiently on 60 Hz.
Another example is an adjustable frequency motor drive. As the frequency is reduced, so is the voltage. Otherwise the current would be excessive and burn the motor out.
 
What are the pros/cons of 60Hz and (what was it) 440Hz?
 
The phenomenon of mutual induction (a.k.a. back EMF) between conductors in a transformer (or motor) winding is what limits the current. A very large utility distribution transformer will have 735 Kv on a primary winding of only a few ohms resistance. (0 ohms if they could make it). The equipment is designed to work efficiently on 60 Hz.
Another example is an adjustable frequency motor drive. As the frequency is reduced, so is the voltage. Otherwise the current would be excessive and burn the motor out.

Wow, that seems logical. Thank you so much. :biggrin:
 
Arctic Fox said:
What are the pros/cons of 60Hz and (what was it) 440Hz?

Almost all motors and power transformers use a core of laminated steel to conduct magnetism. The iron molecules line up according to the direction of the magnetic lines, which is decided by the electrical polarity. There's a slight hesitation of the molecules to follow the (constantly reversing) magnetism called hysteresis, which is energy loss. At 60 Hz the loss is small but increases with frequency.
A 2 pole induction motor will spin at 3500 rpm at 60 Hz so 400 Hz is used to run special motors at higher speeds. For even higher frequencies into the MHz range, ferrite is used in place of iron.
 
Very basic question. Consider a 3-terminal device with terminals say A,B,C. Kirchhoff Current Law (KCL) and Kirchhoff Voltage Law (KVL) establish two relationships between the 3 currents entering the terminals and the 3 terminal's voltage pairs respectively. So we have 2 equations in 6 unknowns. To proceed further we need two more (independent) equations in order to solve the circuit the 3-terminal device is connected to (basically one treats such a device as an unbalanced two-port...
Thread 'Weird near-field phenomenon I get in my EM simulation'
I recently made a basic simulation of wire antennas and I am not sure if the near field in my simulation is modeled correctly. One of the things that worry me is the fact that sometimes I see in my simulation "movements" in the near field that seems to be faster than the speed of wave propagation I defined (the speed of light in the simulation). Specifically I see "nodes" of low amplitude in the E field that are quickly "emitted" from the antenna and then slow down as they approach the far...
Back
Top