Pulse Width of a Magnetic Field

In summary, the conversation discusses calculating the period of a transient DC magnetic field from a half sine wave magnetiser output into an air core wirewound coil. The individual provides information on the coil resistance, inductance, and connecting cable size and lengths. They also mention the uncertainty in calculating the resonant frequency and ask for guidance on measuring the pulse width directly from the coil during the magnetic pulse. They also discuss using 25000 uF capacitors and a Hall Probe to verify the magnetic field. The conversation ends with a mention of reaching 11,200 amperes in testing the saturation of the magnet and concerns about reverse polarity magnetization.
  • #1
Nash78
20
0
Hello, new kid on the block here.
I have read the rules and hereby present my question.

My aim is to calculate the period of a transient DC magnetic field from a half sine wave magnetiser output into an air core wirewound coil.

Coil Resistance : 14.66 mili ohms (derived using voltage drop by passing 1A of DC current into the coil)

Inductance : ~295 micro henries (measured via inductance meter)

Connecting cable size and lengths : 50mmsq and a total of 6meters (I assume that to be of negligible resistance and inductance for my equation)

Magnetiser resistance and inductance : No idea on how to get that, because the manufacturer does not supply.

Magnetiser capacitance : 25 mili farads

So, basically it is a R-L-C circuit in simplicity. With all the information i have on hand, my calculations come up to around 26 msecs.
But i am not confident of my results, as the formula i used, is to calculate the resonant frequency. This is something i am pretty unsure of, even after checking some technical papers online.

1) Is the resonant frequency = pulse width of the magnetic field? Confused... as the manufacturer of the magnetiser explains the output will be only a half-sine wave. I understand the word "resonant", as a oscillating wave which goes up/down until the amplitude disappears as energy is lost through each oscillation.

2) Can anyone guide me on how to measure the pulse width directly from the coil during the magnetic pulse? I have studied basic electrical engineering and understands my fluke multi-meter measures via high resistance inputs. But the reality of the magnetiser current displaying in excess of 10 kilo-amperes per pulse scares me in performing "live" measurements.

Kind souls, please guide me using simple explanations.:shy:
 
Engineering news on Phys.org
  • #2
Using 25000 uF and 295 uH I get a resonant frequency of 58.61 Hz. This frequency has a period of 17 mSec.

However, the reactance of the components at resonance is only 0.11 ohms so you may not notice any resonance at all.

If it is a sinewave, you would get opposite magnetization on each half cycle of the sinewave assuming you used repeating cycles. But it would be roughly sinusoidal in shape, so the field would also be varying in amplitude. Each half cycle would have a period of 17 / 2 or 8.5 mSec.

25000 uF capacitors would invariably be electrolytic, so they may need some DC voltage on them to maintain the integrity of the capacitors.

To verify the magnetic field, you would probably use a Hall Probe. Several good Hall Probe chips are available with built-in amplifiers.

10000 AMPS! Are you sure about this? What are you doing?

.
 
  • #3
vk6kro said:
Using 25000 uF and 295 uH I get a resonant frequency of 58.61 Hz. This frequency has a period of 17 mSec.

However, the reactance of the components at resonance is only 0.11 ohms so you may not notice any resonance at all.

If it is a sinewave, you would get opposite magnetization on each half cycle of the sinewave assuming you used repeating cycles. But it would be roughly sinusoidal in shape, so the field would also be varying in amplitude. Each half cycle would have a period of 17 / 2 or 8.5 mSec.

25000 uF capacitors would invariably be electrolytic, so they may need some DC voltage on them to maintain the integrity of the capacitors.

To verify the magnetic field, you would probably use a Hall Probe. Several good Hall Probe chips are available with built-in amplifiers.

10000 AMPS! Are you sure about this? What are you doing?

.

Hmmm, yours and mine have different values of the resonant frequency.

We are getting a reading of actually 11,200 amperes from the display of the magnetiser.
This is only a transient current, not a steady state current. So the coil does not blow in my face when i pump the current in.:smile:

From my own understanding, this is how the thing works. The magnetiser "pumps" all the charged energy from the capacitors into the coil. The pulse width is limited by all the R + L + C of the entire setup. The manufacturer claims it is only ONE half sine wave, either positive of negative, depending on how we connect the output cables.

So it means all the energy has to be expended into the coil in that half sine cycle.

We reached this value of 11,200 amperes by testing the saturation of the magnet. The magnet only seems to hit saturation at this current and above. Currently, this is the only way of doing without any measurement instruments to determine the gauss value of the field.
 
  • #4
See thumbnail. I used 1000 volts. Max current in coil ~ 8,500 amps.
 

Attachments

  • RLC_Pulse3.jpg
    RLC_Pulse3.jpg
    49.6 KB · Views: 421
Last edited:
  • #5
Hi Nash-
This is a follow-up to my previous post.
First, in my thumbnail, the black curve is voltage, use vertical scale on left. The red curve is current, use vertical scale on right.
The calculated resonant frequency is (1/2 pi)*(1/sqrt(LC)) = 58.6 Hz. The calculated half-cycle time is 8.5 millisec, about what is seen in my posted thumbnail.
Make sure you have included all losses, such as capacitor internal series resistance. You might have to look at the capacitor itself, get mfgr and type, and look on internet.
Is the capacitor unipolar or bipolar? Does it have a reverse diode on it to block reverse voltages such as seen in my thumbnail. Lastly, note that the second reverse polarity pulsed current peak (at about 16 msec) will reverse magnetize your sample. Are you concerned about reverse polarity magnetization, and whether it might demagnetize your sample?
Bob S
 
  • #6
Bob S said:
Hi Nash-
This is a follow-up to my previous post.
First, in my thumbnail, the black curve is voltage, use vertical scale on left. The red curve is current, use vertical scale on right.
The calculated resonant frequency is (1/2 pi)*(1/sqrt(LC)) = 58.6 Hz. The calculated half-cycle time is 8.5 millisec, about what is seen in my posted thumbnail.
Make sure you have included all losses, such as capacitor internal series resistance. You might have to look at the capacitor itself, get mfgr and type, and look on internet.
Is the capacitor unipolar or bipolar? Does it have a reverse diode on it to block reverse voltages such as seen in my thumbnail. Lastly, note that the second reverse polarity pulsed current peak (at about 16 msec) will reverse magnetize your sample. Are you concerned about reverse polarity magnetization, and whether it might demagnetize your sample?
Bob S

Hi Bob, i appreciate the follow-up. I have done quite some homework before on a magnetizer, especially what the manufacturer has told me. We have on hand a Sine-Half Wave Magnetizer, which typically produces only a half sine wave magnetic pulse to any connected coil.

The magnetiser internal inductance and resistance is unknown. This information is not disclosed to us nor will it ever be ( i think...). I have absolutely no idea on how to perform my own measurements to get them.

From the schematics, there is a diode in series with a scr, connected to one of the outputs. So the answer to your question, it should be a YES, there is a diode to block the reverse polarity. The capacitors are bipolar and there is NO label on the caps, so no way to know who manufactured them too.

I just hope that i am not going in the wrong direction :tongue:
 
  • #7
Hi Nash-
I put a generic diode in, and it seemed to work. See thumbnail. Black is coil voltage, left scale. Red is current, right scale. Blue is capacitor voltage, left scale.
NOTE that there is voltage left on the capacitor after the pulse.
Bob S
 

Attachments

  • RLC_Pulse5.jpg
    RLC_Pulse5.jpg
    43.9 KB · Views: 364
  • #8
Dear Bob,

Your example makes perfect sense.

SO all the calculations have been right! Maybe i should have better confidence in what i am doing...

All i need to do is to get the resonant frequency and divide it by 2.
Amplitude just depends on the voltage upon the pulse into the coil, that is for the later part which i will try to calculate how much heat my coil dissipates at each pulse.

I greatly appreciate your help! And in return, i will post my later findings for sharing with the rest of the forum members.

PS: Is your software freeware or those expensive ones?

Rgds
Nash
 
  • #9
Hi Nask-
1) To get the pulse width of half cycle, calculate resonant frequency, get reciprocal to get period, then divide period by two.

2) To estimate the peak coil current, equate stored energy in capacitor and in coil:

(1/2)CV2 = (1/2)LI2
Using C=.025 F, V=1000, and L = 295 uH. I get 9205 amps peak.

3) Software is FREE! I am using LTspice IV from www.linear.com.

Bob S
 
  • #10
Hi Bob,

Im beginning to use LT Spice, is there any transformer and bridge rectifier component somewhere? I can't seem to find them.

Thanks to you, I'm completing my work soon.
Really appreciate the help. :redface:

Rgds,
Nash
 
  • #11
High Nash-
For a bridge rectifier, I would use 4 generic diodes, or you can choose a specific diode from a list. I have not tried it, but for transformers, you use a spice directive and two inductors (with the polarity circle) back to back. The relative inductance is the turns ratio squared. See HELP in the top toolbar, then type "transformer" in the search box.
Bob S

[Edit] I added the attached thumbnail jpg showing a 10:1 (120 volt to 12 volt) transformer using a spice directive (under Edit in top LTspice toolbar).
Bob S
 

Attachments

  • Transformer1.jpg
    Transformer1.jpg
    41.4 KB · Views: 430
Last edited:

1. What is pulse width of a magnetic field?

Pulse width of a magnetic field refers to the duration of time during which a magnetic field is present. It is typically measured in seconds and is an important factor in understanding the behavior and effects of magnetic fields.

2. How is pulse width of a magnetic field measured?

Pulse width of a magnetic field can be measured using specialized equipment such as oscilloscopes, which can detect changes in magnetic fields over time. Another method is to use mathematical calculations based on the frequency and amplitude of the magnetic field.

3. What factors can affect the pulse width of a magnetic field?

The pulse width of a magnetic field can be affected by several factors, including the strength and amplitude of the magnetic field, the frequency of the field, and the material or medium through which the field is passing.

4. Why is pulse width of a magnetic field important to study?

Studying the pulse width of a magnetic field can provide valuable insights into the behavior and effects of magnetic fields on various materials and systems. It can also help in understanding the mechanisms behind electromagnetic induction and other phenomena related to magnetic fields.

5. How can pulse width of a magnetic field be controlled or manipulated?

The pulse width of a magnetic field can be controlled or manipulated by adjusting the frequency and amplitude of the field, as well as using materials with different magnetic properties. Electromagnets can also be used to create and control magnetic fields with specific pulse widths.

Similar threads

Replies
4
Views
1K
Replies
7
Views
3K
  • Electrical Engineering
Replies
4
Views
5K
  • Classical Physics
Replies
4
Views
995
Replies
4
Views
1K
Replies
13
Views
2K
  • Electromagnetism
2
Replies
40
Views
2K
Replies
1
Views
2K
  • Electrical Engineering
Replies
1
Views
994
Replies
41
Views
3K
Back
Top