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On Mon, 10 Jun 2024 00:29:17 -0000 (UTC), Phil Hobbs <pcdhSpamMeSenseless@electrooptical.net> wrote:
>JM <sunaecoNoSpam@gmail.com> wrote:>On Sun, 9 Jun 2024 18:09:24 -0000 (UTC), Phil Hobbs>
<pcdhSpamMeSenseless@electrooptical.net> wrote:
Jeroen Belleman <jeroen@nospam.please> wrote:On 6/9/24 19:02, ehsjr wrote:On 6/7/2024 9:14 PM, JM wrote:A collection of monographs on high accuracy electronics written by Mr.
Chris Daykin, following his career predominantly in metrology.
Unfortunately Chris will be unable to complete the unfinished
monographs (having started end of life care) but there is plenty of
interest to any analogue engineer.
https://1drv.ms/b/c/1af24d72a509cd48/EZhO_rP5-glDmxtc4ZHycvYBhrsqmyC5tuZjt2NFFsS0gQ?e=Wq2Yj0
Thanks!
Ed
I have an issue with his definition of resistor noise power
as the product of open-circuit noise voltage and short-circuit
current. That makes no sense.
There's more than that, probably, but that just jumped out at
me.
Jeroen Belleman
It?s four times too high, for a start.
Cheers
Phil Hobbs
"It is shown elsewhere [1] that the noise power is four times the heat
energy which would flow down the conductors
from a warm source resistor to a matching cold resistor."
Which, if true, would solve all our energy problems, except that
thermodynamic systems would all be unstable.
>
The thermal noise power produced by a resistor into a matched load is kT
per hertz.
>
Cheers
>
Phil Hobbs
Sure, which is what he states. By mentioning a hot and cold resistor he makes it clear that net energy flow is from hot to cold, and that the T refers to the hot source.
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