E
Eeyore
- Jan 1, 1970
- 0
Jim said:QED: Eeyore has been proven incompetent ;-)
Pppfffttttt !
I was on the right track !
Graham
Jim said:QED: Eeyore has been proven incompetent ;-)
Eeyore said:Terry Given wrote:
Eh ? Q . t^-1 = I
OK. Neat trick. Hadn't figured that one.
Just the rate. Of course it it was very slow the gate would never charge to V.
Interesting.
Graham
Terry said:LOL. I cant read....
correct, and the analysis then gets slightly harder.
HTH
next interesting question: what about using a bipolar drive (+/-15V) and
resistor? I'll leave the analysis as an exercise for the interested reader
dated Wed said:During a vacation job back in the college days I build many of these.
About the size of a Westinghouse fridge when complete. I guess they are
still doing their job in locomotives (in Brazil).
Jim said:QED: Eeyore has been proven incompetent ;-)
...Jim Thompson
The gate resistors are in series with the gates but they are all driven
from a single source.
My test stratgey is:
1 - ground the common signal source
2 - apply an appropriate pulse at the test point beween one Fet and its
gate resistor
3 - acquire the Vds data (gppib data from oscioscope) before during and
after the "appropriate gate pulse"
4 - crunch Vds to see that the correct "dip" is there for a Fet sinking
some current.
dont bother, its wrong. The basic maths is:
E = 0.5*Q*V = 0.5*C*V^2
P = E*f
do a dimensional analysis (IOW look at the units) of your equation, they
dont match.
When you put 0.5*C*V^2 J into a cap thru a resistor, the resistor also
dissipates 0.5*C*V^2 J. When you then discharge the cap into the same
resistor, again it dissipates 0.5CV^2 J, leading to a total resistor
energy loss of CV^2 J to charge C to V Volts then discharge C. Repeat at
some frequency F, and voila: P = CV^2F
The resistor doesnt appear in the equation because it is not controlling
the voltage to which the cap gets charged.
The above assumes the cap is both fully charged and discharged.
Eeyore said:Sounds sensible.
Which voltage ?
This all sounds a bit arse about face to me.
Graham
John said:It also assumes that the drive is much faster than the tau of the
resistor*gate capacitance.
John
They're both incompetent because the MOSFET Cin is nonlinear, time
varying, and a complicated function of gate driver performance. It is
not necessary to compute the gate resistor power dissipation to any
great accuracy, it is only necessary to bound it. The gate resistor
power handling will usually be derated by a factor of two minimum. A
more usable estimate simply works on worst-case rise and fall times of
Vgs, derived from manufacturer total gate charge requirements and driver
characteristics, like so:
View in a fixed-width font such as Courier.
.
.
. 2
. (Vin-Vgs) Vin
. P (t)= --------- & Vgs= --- x t
. R R Tr
.
. 2 Tr
. V / 2
. in | t 2 Vin Tr
. -> E = --- * | (1 - --) dt = --- * --
. R R | Tr R 3
. /
. 0
. 2
. Vin Tf
. Similarly on fall E = --- * --
. R R 3
.
.
.
. 2
. Vin
. P = --- x F x T , T = Tr + Tf , F=frequency
. R,AVG 3R T T
.
.
.
I don't know that I'd describe Cin as "non-linear", but you have a
point. There is a region where the gate "eats" charge, but doesn't
change voltage. I suspect you can analyze the power dissipated in a
far simpler fashion than you suggest.
In message <[email protected]>, dated Thu, 31
If the device model is good, LT Spice will tell you what the dissipation
in the resistor is.
Fred said:That so-called test is not representative of any actual circuit stress
on the gate resistors. A simple calculation, as in my first post, shows
that the average power dissipation in the gate resistor is inversely
proportional to Rg and directly proportional to the transition times. If
the transition times are proportional to RgxCin, as one might expect,
then the average power dissipated in Rg is independent of Rg and in
direct proportion to a F*Cpd*Vg^2 product, where Cpd is a parameter
similar to that specified for the CMOS logic families as a means to
estimate power dissipation with frequency. The reason why a Cpd cannot
be universally applied to power MOSFETs is that Cpd will be load
dependent. As others have stated, it may not be power so much as peak
current handling capability of the Rg that is in question.
Hello John,
Don't discount pulse load limits. Metal film types exhibit certain
pathologies related to that. That is a serious concern with most of
my ultrasound pulser designs. I used to prefer Beyschlag because of
their excellent specsmanship. They were bought by Vishay but much of
the info is now online: http://www.vishay.com/docs/49280/tn0006.pdf
They are also very helpful on the phone but if it's still like it
used to be, ideally you'd have to be able to speak German. Preferably
with a northern accent ;-)
Capability" circa Thurs, Feb 26 2004 :
"This is a common reliability problem with power electronics -
"designers"
often neglect peak pulse power in MOSFET gate resistors - I saw one
design
with 4.7Ohm Rg, +12V Vg i.e. 31W peak, using 0805 resistors that failed
after a short time, causing catastrophic failure; so much damage was
done
each time that the root cause was totally obscured, and the "designer"
could
not stop it happening. oops. "
I am the lowly test engineer with the 10 fets in parallel test question
from several months ago. I the process of getting my head around how
hard I can pulse my 10 ohm gate resistors when one side itied to
ground. I read Terry's above note.
Anyone care to elaborate or point me to a good app note regarding
sizing Mosfet gate resistors?
The board I am testing (yes "they" decided the mosfets need to be
individually turned on. . .I knew "they" would) looks suspicously like
"oops".
They're both incompetent because the MOSFET Cin is nonlinear, time
varying, and a complicated function of gate driver performance. It is
not necessary to compute the gate resistor power dissipation to any
great accuracy, it is only necessary to bound it. The gate resistor
power handling will usually be derated by a factor of two minimum. A
more usable estimate simply works on worst-case rise and fall times of
Vgs, derived from manufacturer total gate charge requirements and driver
characteristics, like so:
View in a fixed-width font such as Courier.
.
.
. 2
. (Vin-Vgs) Vin
. P (t)= --------- & Vgs= --- x t
. R R Tr
.
. 2 Tr
. V / 2
. in | t 2 Vin Tr
. -> E = --- * | (1 - --) dt = --- * --
. R R | Tr R 3
. /
. 0
. 2
. Vin Tf
. Similarly on fall E = --- * --
. R R 3
.
.
.
. 2
. Vin
. P = --- x F x T , T = Tr + Tf , F=frequency
. R,AVG 3R T T
Instinctively I'd treat it as equivalent to 30V unipolar.
Since an effective transition time is an RMS of the two, the driver need
only transition ~10x faster to make its contribution negligible. This is
a reasonable constraint for specialized driver ICs and most worthwhile
improvised substitutions.
A typical SMD resistor seems much more fragile than the older
already-fragile film resistors.
It looks like some engineers aren't taking the conservative
peak-power specs typically found in a data sheet seriously,
perhaps because they got used to better in the old days.
Those "professional thin film MELF resistors" look impressive.
Do you have any specific data on peak-power vs time profiles in
cases where you got into trouble with ordinary SMD parts?
Yep, ANY SPice will calculate it correctly IF the model is good...
PSpice Level=7, or HSpice Level=28 or Level=49