RC Networks
While perusing through volume one of Chestnut and Mayer's Servomechanisms and Regulating System Design
(John Wiley & Sons, New York, second edition, 1959)
I came across an interesting table on page 560 (the same table is also in Korn and Korn's Electronic Analog and Hybrid Computers from 1964, another
McGrawHill publication, as Table A1 on page 553). At the bottom of the table was the attribute to the origin of
this table: an article in the April 1952 edition of Electronics magazine, published by McGrawHill.
As luck would have it, the American Radio History website has a scanned copy of that magazine:
Electronics, McGrawHill, April 1952.
And there on page 147 (155 of the PDF) is the original table (Table 1) at the end of an article on
Driftless DC Amplifiers by Frank Bradley and Rawley McCoy of Reeves Instrument Corp, New York, NY,
the table itself apparently the work of their colleague S. Godet.
So, what's all the fuss about something from 66 years ago? Take a look: here's the table from that magazine article:
Table 1: Transfer Functions of RC Input and Output Networks.
What an interesting treasure trove of RC networks. Some familiar, some not so familiar. And all catalogued complete with expressions
describing their function.
In Godet's table the networks were grouped by transfer impedance functions. We could also group them by the network configuration and their conjugate,
swapping R and C. For example, take the single R  it's conjugate would be the single C. Some network configurations would not have a natural conjugate,
for example the R and C in parallel or in series  swapping the R and C would produce the exact same network.
The full title of these transfer functions is "shortcircuit transfer impedance functions". This means that the functions
relate the input voltage to the output current into a shortcircuit. Which is exactly what is required for circuit blocks based
on the virtualearth inverting opamp circuit:
Here, the input pin to the amplifier is driven to be zero volts (virtual earth) by the feedback path around the amplifier through \(Z_o\),
precisely cancelling any currents flowing in through \(Z_i\).
The transfer function \(\frac{V_{out}}{V_{in}}\) is the wellknown \(\frac{Z_o}{Z_i}\). Given a desired transfer function we can then split it
into two parts for \(Z_o\) and \(Z_i\) and then consult the table to find suitable RC networks.
It is interesting to
note that when the paper was published the notation of the time was to use p (or sometimes P) as the complex frequency variable,
compared to today where s (the Laplace operator) is used. In this case they can be used interchangably, so for p read s
to get to something that looks more familiar.
On this page, over time, I will be cataloguing each of these circuits, as well as providing further information about them, such as DC paths
(useful for setting up bias conditions).
ID 
Transfer Impedance Function 
Network 
Relations 
Inverse Relations 
1 
$$A$$ 

$$A = R$$ 
$$R = A$$ 
2 
$$\frac{A}{1+sT}$$ 

$$A = R$$ $$T = RC$$ 
$$R = A$$ $$C = \frac{T}{A}$$ 
