Calculating Current from a Function Generator

AI Thread Summary
To calculate current from a function generator for a magnetic field experiment, a small resistor can be placed in series with the coil, allowing measurement of voltage across the resistor to determine current using I=V/R. Given the high frequency of 15 MHz, it's crucial to ensure the coil is not self-resonant, which can be checked by varying the frequency. The equation I = Vpp/(2Rf) can be used to calculate current, factoring in the peak-to-peak voltage (Vpp) and frequency (f). Additionally, the duty cycle of the pulse bursts must be considered, leading to the modified equation I = (Vppd)/(2Rf). Finally, the magnetic field can be calculated using B = μ0IN, where I is the current calculated.
Student1008
Messages
2
Reaction score
0
I wasn't sure where to post this, but I am a physics student working on a thesis and the experiment I ran involved using a function generator to generate a magnetic field (wire was bent into a loop). I am trying to figure out how to convert the frequency (15 MHz) and Vpp (10V) to current so I can calculate the B-field. I know it's not as simple as V = IR since it's a wave (pulse bursts to be exact). Please help!
 
Engineering news on Phys.org
Hi
If you want to measure the current through a coil then you can put a small Resistor in series (at the Earthy End would be easiest) and look at the volts across that. The current through your coil will then be I=V/R. If the current is really high then your resistor can be very low and still give you a measurable voltage drop across the resistor. This is just what a DVM does, in fact, when measuring current.
The high frequency involved could be a problem here, though, if the coil has multiple turns and could be self-resonant. This can be detected by varying the frequency and checking that the current is just dropping linearly from 0 to 15MHz - i.e you are off resonance. It would dip sharply at a parallel resonance.
 
sophiecentaur said:
Hi
If you want to measure the current through a coil then you can put a small Resistor in series (at the Earthy End would be easiest) and look at the volts across that. The current through your coil will then be I=V/R. If the current is really high then your resistor can be very low and still give you a measurable voltage drop across the resistor. This is just what a DVM does, in fact, when measuring current.


Is this the only way to measure the current? I was also thinking of trying to formulate a wave equation from the frequency/B-field (I am studying magnetoinductive waves). Would you have an idea of how to do that?
 
You can also use a hall sensor to measure current, assuming your test setup is still in place.
 


As a fellow scientist, I understand your dilemma and am happy to provide some guidance on how to calculate current from a function generator.

First, it is important to note that the equation V = IR still applies in this scenario, but we need to consider the time-varying nature of the signal being produced by the function generator. This means that we need to take into account the frequency and pulse bursts in our calculations.

To calculate the current, we can use the following equation: I = Vpp/2R, where Vpp is the peak-to-peak voltage and R is the resistance of the wire loop. However, since the frequency of the signal is 15 MHz, we also need to consider the time component. The equation for calculating current in this case would be: I = Vpp/(2Rf), where f is the frequency in Hertz.

Now, since the signal from the function generator is a pulse burst, we need to consider the duty cycle, which is the ratio of the pulse duration to the total period. This can be represented as a percentage or decimal. For example, if the pulse duration is 1 ms and the total period is 10 ms, the duty cycle would be 10%.

To account for the duty cycle, we can modify our equation to be: I = (Vppd)/(2Rf), where d is the duty cycle.

Finally, to calculate the B-field, we can use the equation B = μ0IN, where μ0 is the permeability of free space, I is the current we just calculated, and N is the number of turns in the wire loop.

I hope this helps you in your calculations and in your thesis. Best of luck with your experiment!
 
While I was rolling out a shielded cable, a though came to my mind - what happens to the current flow in the cable if there came a short between the wire and the shield in both ends of the cable? For simplicity, lets assume a 1-wire copper wire wrapped in an aluminum shield. The wire and the shield has the same cross section area. There are insulating material between them, and in both ends there is a short between them. My first thought, the total resistance of the cable would be reduced...
Hi all I have some confusion about piezoelectrical sensors combination. If i have three acoustic piezoelectrical sensors (with same receive sensitivity in dB ref V/1uPa) placed at specific distance, these sensors receive acoustic signal from a sound source placed at far field distance (Plane Wave) and from broadside. I receive output of these sensors through individual preamplifiers, add them through hardware like summer circuit adder or in software after digitization and in this way got an...
I am not an electrical engineering student, but a lowly apprentice electrician. I learn both on the job and also take classes for my apprenticeship. I recently wired my first transformer and I understand that the neutral and ground are bonded together in the transformer or in the service. What I don't understand is, if the neutral is a current carrying conductor, which is then bonded to the ground conductor, why does current only flow back to its source and not on the ground path...
Back
Top