M
Michael
Hi there - I was looking at the high voltage video flyback converter
(page 374, figure 6.55A) in art of electronics. I feel like I
understand most of it, but I want to clarify a couple things just to
be sure:
First of all, I'm only really comfortable with transformers being used
to take AC in and spit AC out. That's really all I've ever been taught
to do with them. Their full functionality was never really explained,
nor their makeup, or anything else. Essentially I was taught Vs/Ns =
Vp/Np. Thinking about it though, am I right in thinking that a
transformer is essentially an inductor that has multiple paths for
current to flow? Or in other words, when one inductor in a transformer
has a certain amount of energy stored, that energy is shared between
both the primary and secondary and can be used to create a current
through either the primary or the secondary.
Like in figure 6.55A - this is what I'm thinking: Q1 turns on and the
primary coil reaches some high current and then Q1 turns off. A
significant amount of energy has been stored in the transformer, so it
does what it can to continue a current flow. It can't make any current
flow in the primary, but the secondary does have a path for current,
so current flows through there. Would the voltage across the secondary
then be Ls*(dip/dt)? (where Ls = inductance of secondary, and dip/dt
is the derivative of the current through the primary). Since Ls is
much larger than Lp, this is going to be a very large voltage.
Additionally, if C1 were already at a very high voltage, D1 is there
to protect Q1 so that the collector of Q1 won't see above about 300VDC
(as the voltage across the primary will increase trying to get current
to flow through it). D2 is there so that the transformer can only
charge C1, not drain it as well. D3 is there to protect the collector
from going too far negative when Q1 is first turned on.
How far off am I?
Thanks!
-Michael
(page 374, figure 6.55A) in art of electronics. I feel like I
understand most of it, but I want to clarify a couple things just to
be sure:
First of all, I'm only really comfortable with transformers being used
to take AC in and spit AC out. That's really all I've ever been taught
to do with them. Their full functionality was never really explained,
nor their makeup, or anything else. Essentially I was taught Vs/Ns =
Vp/Np. Thinking about it though, am I right in thinking that a
transformer is essentially an inductor that has multiple paths for
current to flow? Or in other words, when one inductor in a transformer
has a certain amount of energy stored, that energy is shared between
both the primary and secondary and can be used to create a current
through either the primary or the secondary.
Like in figure 6.55A - this is what I'm thinking: Q1 turns on and the
primary coil reaches some high current and then Q1 turns off. A
significant amount of energy has been stored in the transformer, so it
does what it can to continue a current flow. It can't make any current
flow in the primary, but the secondary does have a path for current,
so current flows through there. Would the voltage across the secondary
then be Ls*(dip/dt)? (where Ls = inductance of secondary, and dip/dt
is the derivative of the current through the primary). Since Ls is
much larger than Lp, this is going to be a very large voltage.
Additionally, if C1 were already at a very high voltage, D1 is there
to protect Q1 so that the collector of Q1 won't see above about 300VDC
(as the voltage across the primary will increase trying to get current
to flow through it). D2 is there so that the transformer can only
charge C1, not drain it as well. D3 is there to protect the collector
from going too far negative when Q1 is first turned on.
How far off am I?
Thanks!
-Michael