From: kevin93 on
On Dec 18, 12:48 pm, D from BC <myrealaddr...(a)comic.com> wrote:
> On Fri, 18 Dec 2009 07:54:13 -0800 (PST), "J.A. Legris"
.... right? Try adjusting the little screw on the probe.
>
> frick!
> That's it!
> Adjusting the probe comp screw is the only thing to affect the area of
> interest.
>
> Vds is yellow trace.
> Green trace is my other probe deliberately put out of calibration(more
> than what is was) to emulate out of cal probe 1.
> Green is on the cali pulse out on the scope and due to f diff I waited
> for the signal to float by for stopping the acquisition.
>
> http://members.shaw.ca/chainsaw/SED/vdsandprobenotcali
> 40k PNG and in color!
>
> I suppose if I had a fet probe/active probe, Vds would look more like
> as seen on a simulator.
> That or I learn how to discern what's probe signal and what's circuit
> signal.
>
> groan.. :(
>
> Thanks

You also have to be careful about scope overload when looking at this
type of thing. Many scopes can take a long time to recover from the
overload that occurs "off-screen"

kevin

From: krw on
On Thu, 17 Dec 2009 22:07:01 -0800, Archimedes' Lever
<OneBigLever(a)InfiniteSeries.Org> wrote:

>On Thu, 17 Dec 2009 12:53:43 -0800 (PST), "langwadt(a)fonz.dk"
><langwadt(a)fonz.dk> wrote:
>
>>On 17 Dec., 20:17, D from BC <myrealaddr...(a)comic.com> wrote:
>>> I got a 10 ohm carbon switched by a mosfet(TO-220).
>>> Spec sheet: Rdson=0.17ohms at 9.8amps with <=300uS pulse 2% duty.
>>> R to drain.
>>> Source to gnd.
>>> 20V regulated supply
>>>
>>> On the scope I've noticed that Vdson is still increasing in voltage
>>> (Ids still increasing) after a 50uS mosfet turn on time.
>>> (Freq=10xper second.)
>>> I do spot the initial current signature due to loop inductance but
>>> following that Id morphs to a slope too gradual to be inductance.
>>> Id levels off and stays constant after about 100uS.
>>>
>>> Is it thermal?
>>> Is the mosfet material is heating up and becoming more resistive?
>>> Then it's able to cool down before the next pulse..
>>>
>>> If it's a thermal dynamic, then I suppose this may not show up on a
>>> simulator.
>>
>>have a look at the datasheet for a random mosfet, look for tj vs. Ron
>>looks like it generally doubles from 20C to 100C
>>
>>
>>-Lasse
>
> For really good devices check out Zetex.

AlwaysWrong, DI bought them out some time back and ditched a lot of
the nice stuff.
From: John Larkin on
On Thu, 17 Dec 2009 11:17:15 -0800, D from BC
<myrealaddress(a)comic.com> wrote:

>I got a 10 ohm carbon switched by a mosfet(TO-220).
>Spec sheet: Rdson=0.17ohms at 9.8amps with <=300uS pulse 2% duty.
>R to drain.
>Source to gnd.
>20V regulated supply
>
>On the scope I've noticed that Vdson is still increasing in voltage
>(Ids still increasing) after a 50uS mosfet turn on time.
>(Freq=10xper second.)
>I do spot the initial current signature due to loop inductance but
>following that Id morphs to a slope too gradual to be inductance.
>Id levels off and stays constant after about 100uS.
>
>Is it thermal?
>Is the mosfet material is heating up and becoming more resistive?
>Then it's able to cool down before the next pulse..
>
>If it's a thermal dynamic, then I suppose this may not show up on a
>simulator.

100 us sounds fast to be thermal. But could be.

Lots of scopes recover poorly from gross overloads.

Scope probe compensation?

John

From: D from BC on
On Fri, 18 Dec 2009 00:05:03 -0800 (PST), Bill Sloman
<bill.sloman(a)ieee.org> wrote:

>On Dec 18, 5:03�am, D from BC <myrealaddr...(a)comic.com> wrote:
>> On Thu, 17 Dec 2009 15:37:53 -0800, Joerg <inva...(a)invalid.invalid>
>> wrote:
>>
>> >Take a look at figure 4:
>>
>> >http://www.irf.com/product-info/datasheets/data/irfs3806pbf.pdf
>>
>> Yup. Rdson is sensitive to temperature.
>> I'm just surprised to Rdson variation within a 100uS on time.
>> If that's what I'm seeing.
>> That or something goofy somewhere.
>
>The thermal mass of a drain channel isn't all that high. Eventually
>the heat distribution acros the transistor evolves into a nice smooth
>thermal gradient from channel to heat sink, but initially you've got a
>lot of room temperature silicon to take up the first few micro-joules
>of dissipation. Jim might know representative dimensions for drain
>channels.
>
>Silicon has a heat capacity of about 700 joules per kilogram at room
>temperature.
>
>The data sheet suggests limiting avalanche energy to 70 mJ, and stops
>allowing you to increase the single pulse avalanche power for pulse-
>widths below 6usec - which has probably got more to do with the onset
>of channeling than anything specific about the thermal mass of the
>channel.
>
>Figure 13 of the data sheet shows a three-componenet thermal model,
>with the shortest time constant at 260usec, followed by 1.228msec and
>8.12msec. A more physically realistic model, with concentric shells of
>silicon getting warmed up in succession, could probably be resolved
>into exponential components including some with shorter time
>constants.

Figures that I get jammed when the electronics take me into the
semiconductor thermal physics.
As soon I find myself crossing into another field of expertise, that's
when the trouble begins.

From: D from BC on
On Fri, 18 Dec 2009 13:03:25 -0800, Joerg <invalid(a)invalid.invalid>
wrote:

>
>You might get lucky sometimes but I'd still do this on a piece of
>copperclad. Source solder smack to the plane, coax (with divider if
>needed) straight to the scope with it's shield also soldered to the
>plane. I have a bunch of BNC with solder tabs in the drawer for that so
>I can just plug it in. That also takes out any weird effects a probe can
>have.

Getting there..