Modeling a spark gap--How to solve a DE with a step function

Motocross9
Messages
12
Reaction score
4
Homework Statement
I wish to solve a system of differential equations; however, I am modeling a spark gap by using a step function. How could I solve? I'll provide the first equation below as an example:
Relevant Equations
##V_ocos(\omega*t)=\dot Q_1R_1+(Q_2/C_1)(1-U(Q_2-C_1V_o))##
Honestly not sure how to go about this. Again this is one equation of 4 that I have. I considered using Laplace transforms but taking the Laplace transform of a step function whose argument is one of the variables being solved for doesn't seem possible. Also, if there is an alternative way to model a spark gap in a circuit, I would love to be informed of it. Thanks in advance!

(also ##Q_1## and ##Q_2## are the functions of time I wish to solve for)
 
Physics news on Phys.org
Could you post the circuit you're trying to model? The RHS suggests a resistor in series with a capacitor "switched" by the spark-gap. Is that O.K?
 
Gordianus said:
Could you post the circuit you're trying to model? The RHS suggests a resistor in series with a capacitor "switched" by the spark-gap. Is that O.K?
I am modeling the basic Tesla coil circuit. In particular, it is this one:
1597265315096.png

The resistor isn't shown in this diagram, however. I am treating the spark gap as a capacitor, whose voltage drops to zero once the voltage across it reaches ##V_o##. I actually entered the first equation wrong--its fixed now.
 
Quite a tricky circuit. It has, at least, two widely different time constants. A slow one, related to the charge of the HV capacitor at mains frequency and a fast one, related to the discharge of the HV capacitor on the primary of the HV transformer. In a simple model I'd consider the spark gap as a non-linear resistance instead of a capacitor.
 
Hello everyone, I’m considering a point charge q that oscillates harmonically about the origin along the z-axis, e.g. $$z_{q}(t)= A\sin(wt)$$ In a strongly simplified / quasi-instantaneous approximation I ignore retardation and take the electric field at the position ##r=(x,y,z)## simply to be the “Coulomb field at the charge’s instantaneous position”: $$E(r,t)=\frac{q}{4\pi\varepsilon_{0}}\frac{r-r_{q}(t)}{||r-r_{q}(t)||^{3}}$$ with $$r_{q}(t)=(0,0,z_{q}(t))$$ (I’m aware this isn’t...
Hi, I had an exam and I completely messed up a problem. Especially one part which was necessary for the rest of the problem. Basically, I have a wormhole metric: $$(ds)^2 = -(dt)^2 + (dr)^2 + (r^2 + b^2)( (d\theta)^2 + sin^2 \theta (d\phi)^2 )$$ Where ##b=1## with an orbit only in the equatorial plane. We also know from the question that the orbit must satisfy this relationship: $$\varepsilon = \frac{1}{2} (\frac{dr}{d\tau})^2 + V_{eff}(r)$$ Ultimately, I was tasked to find the initial...
Back
Top