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G8MNY > TECH 25.05.07 10:02l 90 Lines 4124 Bytes #999 (0) @ WW
BID : 15856_GB7CIP
Read: GUEST OE7FMI
Subj: PEP Meter modification UPDATE
Path: DB0FHN<DB0NOE<DB0GAP<DB0FSG<DB0MRW<OK0PKL<OK0PPL<DB0RES<IK2XDE<ON4HU<
F4BWT<I0TVL<LA1SFS<GB7CIP
Sent: 070524/2337Z @:GB7CIP.#32.GBR.EU #:15856 [Caterham] $:15856_GB7CIP
From: G8MNY@GB7CIP.#32.GBR.EU
To : TECH@WW
By G8MNY (Update Nov 06)
I was discussing a PEP Power meter project & remembered an old Radcom article
that described the principle of a conversion without much modification & best
of all maintaining calibration. I have now found the article Jan 1989 page 46
& show both my guess at the circuit before I found the article, & my sketch of
the original.
MY GUESS
o Normal
+9V>컴컴컴>o컴컴캑>쳐컴쩡컴�+
PEP LED � ===10u
� _�_ C2
Normal � Normal
o컴컴컴컴컴�)컴컴컴컴컴컴컴컴컴컴컴컴컴컴컴컴컴o
>컴컴>o풮EP �\� PEP�o<컴�> +VE
ORIGINAL 쳐컴쿨컴캑+ \ D1 �\ � ORIGINAL
RF SWR RV1 f.b. � A >컫캑>쳐쩡컴쩡컴컴�+ \ D2 � SWR METER
DETECTORS preset 旼캑- / R2 � 1M � B >컫캑>쳐�
SWITCHING � � �/� 10K � � 旼캑- / R3 �
& CAL POTS � 읕컴�)컴컴)컴컴캑 � � �/ 10K �
� � � u1 === � 읕컴컴컴컴)컴컴켸
� � � C1 � � �
>컴컴컴좔쩡컴컴컴컨컴컴좔컴컴좔컴좔컴컴컴컴컴컨컴컴컴컴�> -VE
_�_
HOW IT WORKS
A 3 pole change over switch, powers up the modification & also switches in the
circuit between the RF detectors & the meter.
Multiturn Preset RV1 has to be set to exactly the same resistance as the meter
is, in practice this can be finely tweeked later on calibration tests.
Opamps A & B must be the FET type that can function correctly with their input
@ 0V (-ve rail). The Ferrite Bead needs to be as close to the opamp input as
possible & in practice may have many turns to eliminate all RF.
R2 puts a slight load on the opamp allowing any slight O/P current to leak
away & not charge up C1. Silicon signal diode D1 allows the opamp only to
charge up C1 (@ 5mA max peak current, hence C1 is a small value to charge
nearly instantly) to the peak +ve voltage the original meter would see from the
detector etc. N.B. This is a very small voltage! But the beauty of opamps is
that they can accurately compare this with the peak input voltage & stop
charging as the precise level.
To discharge the small C1 over a long time relative to audio peaks, 1M is used.
Opamp B then accurately follows the C1 voltage & applies it to the meter.
Again R3 puts a slight load on the B opamp allowing any slight O/P current to
leak away not through the meter. Another silicon signal diode D2 is used to
drop any minimum opamp O/P DC level so that the meter should be able to read
zero OK.
Calibration of RV1 is just to switch between normal & PEP on a steady hum less
carrier & adjust for the identical power reading. Check this at different
power levels & bands.
THE ORIGINAL
D1 旼100k컫컴컫컴컴컴캑<쳐�<+4V to 24V
旼�<쳐캑 � +� 47u D4
_�_ \�/ � === C4
�RV3� � _�_
�50k� �
>컴컴커 1M 1M 3�\�8 IC LM358
ORIGINAL 쳐100k컨쩡�)컴�+ \ 1 D2 5�\
RF SWR RV1 � � � A >캑>쳐100k컫컴컴�+ \ 7 D3
DETECTORS 200 C1� 쳐캑- / � � B >쨈>쳇컴쩡컫�> +VE
SWITCHING � === � 2�/�4 C2 � 旼�- / � � � � SWR
RV2 u1� 쳐컴�)컴캑쳐컴쩡컴캑+ �6�/ � 쿏5� === METER
20K � � � u1 10M === 읕컴컴컴� � _�_ 퀅1
� � 100k � � C3�1u � \_/ 쿎5
>컴컴컨컫컴컴컨컴)컴컴좔컴컴컴컨컴컴좔컴컴컴컴컴컴�)컴좔컨�> -VE
_�_ 읕컴컴컴컴컴컴컴컴컴컴컴컴컴컴컴컴�
What amassed me was my memory of the principles were so exact since 1989!
The man differences are..
1/ The offset pot system RV3.
2/ The heavy RF filtering 100k & C1 (may it affect the AF peaks??)
3/ 1 overall split NFB loop DC 100K & AC though C2, rather than my 2 NFB loops.
4/ Meter overdrive protection diode D5.
5/ I included in out switching & PEP LED.
6/ D5 is an idot diode.
Why Don't U send an interesting bul?
73 de John G8MNY @ GB7CIP
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