Welcome to our site! EDAboard.com is an international Electronics Discussion Forum focused on EDA software, circuits, schematics, books, theory, papers, asic, pld, 8051, DSP, Network, RF, Analog Design, PCB, Service Manuals... and a whole lot more! To participate you need to register. Registration is free. Click here to register now.
Without the resistor, when the transistor turns off, the current through the coil is I (t) = e^(-t*rcoil/L) (ideal diode)
As rcoil/L is generally small, the current fading time can be too long.
Yes, the voltage sources shorts . But that's a current source, which represents an open circuit.
Never say never:
1/Zth = 1/(30-j10) + 1/(40+j20) = (30+j10)/1000 + (40-j20)/2000 = 3/100 + j/100 + 2/100 - j/100 = 5/100 = 1/20
Of course, but has no effect on the current derivative at t=0+
Just think on the standard RLC: Vc + Vr + VL = 0
But VL = L I' = L Vr'/R
then Vc + Vr + (L/R)Vr' = 0
At t=0+ only the instantaneous voltage,current and L/R define Vr'
You start well:
At t=0+
Il = -Ix = 2A
Vc = 16V
Vx = -24V
Vr = 16V
(1) Vr - Vx - Vc + Vl = 0
That's OK.
After that, you derive by entering the second derivative (IL''), something that would lead you to solve the DEQ unnecessarily.
Furthermore, you have almost everything solved...
This site uses cookies to help personalise content, tailor your experience and to keep you logged in if you register.
By continuing to use this site, you are consenting to our use of cookies.