K
Ken Smith
Guest
In article <41AA96A8.B03ABEF8@rica.net>,
John Popelish <jpopelish@rica.net> wrote:
0.1 attoseconds.
(or something like that)
Thermally the situation looks a lt like this:
Power in
= I in R1 R2 R3 R4 R5
-> ---/\/\/\------/\/\/----/\/\/----/\/\----/\/\--- GND
! ! ! ! !
--- --- --- --- ---
--- C1 ---C2 --- C3 --- C4 --- C5
! ! ! ! !
GND GND GND GND GND
C1 is the thermal mass of the actual resistive material.
R1 is the thermal conductivity of the resistive material
C2 is the thermal mass of the substrate the resistive material is on.
R2, R3 with C3, C4 are a lumped constant representation of the substrates
bulk.
C5 and R5 are for the outer package to the air.
Unless you have some feel for R1 and C1 you really can't extrapolate from
1.5 seconds down. I know this because I did it and ended up with 1206
open circuits after a few months of service. The power spike was only
300uS long.
--
--
kensmith@rahul.net forging knowledge
John Popelish <jpopelish@rica.net> wrote:
No, X1.5 applies to 0.1 attoseconds to 1.5 seconds. 1.500001 applies belowHarry Dellamano wrote:
Ken Smith wrote:
IRC (the company, I do Recall Correctly) make some great smt resistors.
And have peak pulse power curves.
Caddock does too:
http://www.caddock.com/Online_catalog/smt/smt.html
--
John Popelish
Caddock is a perfect example of a poor surge (Pulse) power resistor. They
are thin film and X1.5 rated peak power. A good surge rated resistor is
X5000 or maybe 5 Joules. Call Richard Caddock and see if they speak in
Joules.
But that 1.5 factor is allowed for 5 seconds. I was assuming that
from an I^2*t fusing effect that the dissipation capability would go
up quite a bit if the time was in milliseconds.
0.1 attoseconds.
(or something like that)
Thermally the situation looks a lt like this:
Power in
= I in R1 R2 R3 R4 R5
-> ---/\/\/\------/\/\/----/\/\/----/\/\----/\/\--- GND
! ! ! ! !
--- --- --- --- ---
--- C1 ---C2 --- C3 --- C4 --- C5
! ! ! ! !
GND GND GND GND GND
C1 is the thermal mass of the actual resistive material.
R1 is the thermal conductivity of the resistive material
C2 is the thermal mass of the substrate the resistive material is on.
R2, R3 with C3, C4 are a lumped constant representation of the substrates
bulk.
C5 and R5 are for the outer package to the air.
Unless you have some feel for R1 and C1 you really can't extrapolate from
1.5 seconds down. I know this because I did it and ended up with 1206
open circuits after a few months of service. The power spike was only
300uS long.
--
--
kensmith@rahul.net forging knowledge