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G8MNY  > TECH     22.04.04 18:23l 81 Lines 2915 Bytes #999 (0) @ WW
BID : 53941_GB7CIP
Read: GUEST OE7FMI
Subj: An AF amplifier stage
Path: DB0FHN<DB0FOR<DB0MRW<DB0ERF<DB0HDF<DB0HOT<OK0PBX<OK0PAD<OK0PPL<DB0RES<
      ON0AR<GB7CIP
Sent: 040421/2236Z @:GB7CIP.#32.GBR.EU #:53941 [Caterham] $:53941_GB7CIP
From: G8MNY@GB7CIP.#32.GBR.EU
To  : TECH@WW

By G8MNY                                (new graphics Dec 03)
This simple amplifier circuit is easy for calculations.

+9V ÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÂÄÄÄÄÄÄÄÄÄÄÄ
                   Rc
            ÚÄÄÄÄÄÄ´   Cout
           Rb      ÃÄÄÄÄ´ÃÄÄÄÄ
            ³    ³/
I/P ÄÄÄ´ÃÄÄÄÁÄÄÄÄ´ NPN
       Cin       ³\e
                   ³
                   Re
 0VÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÁÄÄÄÄÄÄÄÄÄÄÄ

To get « the DC swing on the O/P then biasing Rb = Hfe x (Rc+Re)
     This is because we want the same voltage CÄE (almost the same as across
     Rb) as across the total load R of Rc+Re.

Gain G approx = Rc/Re  (Rc may be lower due to external load).
     With high Hfe then Ie approx = Ic, so the emitter NFB Re controls the
     collector current making the voltage gain just the voltage drop ratio of
     Rc/Re. Assuming no external loads. For high gain applications Re includes
     the internal emitter R of the transistor (typically a few ohms).

O/P Z = XCout + (Rc // ((GÄ1) x Rb))
     This is the added components, including the apparent fraction of the bias
     Rb with load current in it.
     "//" means in parallel, many of the paralleled terms are insignificant.
     Technically the amount that (G-1)x Rb component that affects the O/P Z
     it will also depend the I/P source Z.  
 
I/P Z = XCin + ((Hfe x Re) // (Rb/(G+1)))
     This is the added components, including the apparent fraction of the bias
     Rb with input current in it.
     "//" means in parallel, many of the paralleled terms are insignificant.

LF Roll off
     Cin & Cout affect the LF response. Basically each one will give Ä3dB &
     6dB/Octave roll off when Xc equals the source + load Zs.

HF Response
     Intrinsically limited by the transistor's FT when the Hfe becomes 1, &
     component layout (inter capacitance) causing Miller HF N.F.B. effects.

HF Compensation
     HF loss can be compensated for by putting a suitable C across Re to give
     +3dB boost were Xc=Re eg where the measure drop is -3dB, & the 6dB/Octave
     lift after that should flatten the amp losses out. The input Z will be
     reduced at HF though. Not often used!


Example

+12V ÄÄÄÄÄÄÄÄÄÄÄÄÄÄÂÄÄÄÄÄÄÄÄÄÄ
                  1Kê
            ÚÄÄÄÄÄÄ´   + Cout
          100Kê    ÃÄÄÄÄ´ÃÄÄÄÄ Output
         +  ³    ³/    0.5uF       ³
I/P ÄÄÄ´ÃÄÄÄÁÄÄÄÄ´ Hfe=100       10K Load
      Cin     NPN³\e               ³
      1uF          ³               ³
                  100ê             ³
 0V ÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÁÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄ

So in the above example Collector should be around +6V
Gain about 9
O/P Z about 900ê +XCout
I/P Z about 5Kê  +XCin

LF response with Input source Z of zero, & O/P load of 10K...
    I/P Ä3dB LF roll off, @ 31Hz where Xc = 5Kê
    O/P Ä3dB LF roll off, @ 29Hz where Xc = 10.9Kê
    Giving Ä6dB @ 30Hz & 12dB/Octave LF cut.

Why don't U send an interesting bul?
/QSL
73 De John, G8MNY @ GB7CIP


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