Hey guys,
(This post is a bit rambly, read and answer at your leisure)
Right now I'm covering RLC circuits. I had a series RLC circuit connected to an oscilloscope and function generator. I used a BNC T splitter on the output of the FG and a BNC to BNC to connect the FG to the scope. I then had a BNC to alligator which connected to the circuit. I then connected my oscilloscope probe to the circuit at the resistor. In the attached scope screen capture the input signal is in blue and the circuit measurement is in yellow. The RLC circuit was made to be underdamped and I saw the nice oscillations in the waveform. I was measuring exactly what I wanted to see out of the circuit which was nice.
However the oscillations in the input were a bit perplexing. It does make some sense to me, I wasn't expecting a nice square wave. I'm curious to know what the ramifications are, and if there is anyway to mitigate these effects on the output signal. Just waving my flashlight around in the dark here
Lastly, I'd like to run my assumptions by you guys. I have a few ideas of why this is happening. I think current is when there is an absence of electrons in one area and that pulls electrons off of the copper in the wire. Those atoms with missing electrons then pull electrons off the atoms near them and so one and so forth up the wire.) I imagine this process has a kind of inertia to it. That is, if electrons stop being pulled off at the... positive side? then the electrons at the "negative" end of the wire wont stop their shuffle at that same instant. I'll come back to this.
Firstly I'd like to look at the instant after the rising edge of the signal. It comes to a peak and then falls off very rapidly. >1µs. I think this is because when the FG switches to its 10V on state the BNC-BNC between the FG and scope is able to rise to 10V initially, but then the RLC circuit begins to draw current which causes the voltage output of the FG to fall because it can't output enough current to charge it and maintain 10V then when one of the components reaches full charge, I'm not sure which, the slope becomes positive. This is where my understanding becomes a little shakier.
After the slope becomes positive the component that built up its charge is now discharging its voltage into the circuit this voltage is then added to the voltage from the FG which causes the voltage to rise above 10V. If I'm not mistaken this is the basis of a boost converter? After the charge of that component is depleted the cycle starts again. This explains the yellow output waveform.
I think these voltage fluctuations are being applied to the FG's output because its not a perfect voltage source (not saying Tek makes bad equipment, just that is has to obey the laws of physics)
Am I anywhere near the target here?
Haha thanks for any light you can shine on this.
(And as you can see from the capture this Oregonian spent 4/20 in the lab. Nerd Life XD)
(This post is a bit rambly, read and answer at your leisure)
Right now I'm covering RLC circuits. I had a series RLC circuit connected to an oscilloscope and function generator. I used a BNC T splitter on the output of the FG and a BNC to BNC to connect the FG to the scope. I then had a BNC to alligator which connected to the circuit. I then connected my oscilloscope probe to the circuit at the resistor. In the attached scope screen capture the input signal is in blue and the circuit measurement is in yellow. The RLC circuit was made to be underdamped and I saw the nice oscillations in the waveform. I was measuring exactly what I wanted to see out of the circuit which was nice.
However the oscillations in the input were a bit perplexing. It does make some sense to me, I wasn't expecting a nice square wave. I'm curious to know what the ramifications are, and if there is anyway to mitigate these effects on the output signal. Just waving my flashlight around in the dark here
Lastly, I'd like to run my assumptions by you guys. I have a few ideas of why this is happening. I think current is when there is an absence of electrons in one area and that pulls electrons off of the copper in the wire. Those atoms with missing electrons then pull electrons off the atoms near them and so one and so forth up the wire.) I imagine this process has a kind of inertia to it. That is, if electrons stop being pulled off at the... positive side? then the electrons at the "negative" end of the wire wont stop their shuffle at that same instant. I'll come back to this.
Firstly I'd like to look at the instant after the rising edge of the signal. It comes to a peak and then falls off very rapidly. >1µs. I think this is because when the FG switches to its 10V on state the BNC-BNC between the FG and scope is able to rise to 10V initially, but then the RLC circuit begins to draw current which causes the voltage output of the FG to fall because it can't output enough current to charge it and maintain 10V then when one of the components reaches full charge, I'm not sure which, the slope becomes positive. This is where my understanding becomes a little shakier.
After the slope becomes positive the component that built up its charge is now discharging its voltage into the circuit this voltage is then added to the voltage from the FG which causes the voltage to rise above 10V. If I'm not mistaken this is the basis of a boost converter? After the charge of that component is depleted the cycle starts again. This explains the yellow output waveform.
I think these voltage fluctuations are being applied to the FG's output because its not a perfect voltage source (not saying Tek makes bad equipment, just that is has to obey the laws of physics)
Am I anywhere near the target here?
Haha thanks for any light you can shine on this.
(And as you can see from the capture this Oregonian spent 4/20 in the lab. Nerd Life XD)
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