Passive Preamplifier

Introduction

The term passive preamplifier is actually a contradiction in terms since it has no amplification. Unlike active preamplifiers, which use a power supply and active components (such as operational amplifiers, transistors, or vacuum tubes) to increase signal strength, passive preamplifiers use exclusively passive components. A passive preamplifier can be described as a pure attenuator with an integrated volume control and input selector. Its main function is to regulate the voltage of the signal without adding any gain or affecting the signal's tonal characteristics.

Advantages

The primary advantage of a passive preamplifier is its lack of active components. This means that it theoretically does not introduce noise, nor total harmonic distortion (THD) or intermodulation distortion (IMD), given that it does not require an external power supply. At the same time, this also reduces the risk of phase errors and overshoot that can occur in active circuits. No power supply means no electromagnetic interference (EMI) or grounding issues, resulting in cleaner signal paths.

Disadvantages

Although passive preamplifiers have many advantages, the absence of active buffering and amplification also introduces technical limitations that must be carefully considered.

Passive preamplifiers can only reduce, not amplify, the signal. This makes them dependent on the source equipment providing sufficient output voltage. In cases where the source has low output voltage, the system may lack the necessary level to drive the power amplifier, especially if the power amplifier has low sensitivity.

Besides lack of amplification, impedance mismatch is often highlighted as a major disadvantage. The figure below shows a schematic representation of the signal path from the source (Tuner, CD etc.) via the passive preamplifier and signal cable to the power amplifier.

In the figure, the resistor RS represents the source resistance from the Tuner, CD etc. in addition to the potentiometer's output resistance. In my own preamplifier I am using a 10 kohm potentiometer. From this potentiometer alone, the maximum setting is 1/4 of 10 kohm: 2.5 kohm.

So this is also the value of the source resistance RS if the output resistance of your Tuner, CD etc is approximately 0 ohms. However, this output resistance will typically be between a few ohms to perhaps 1 kohm. In the latter case the preamplifier will attenuate the signal by about 10/11 times if the power amplifier has an input impedance RL high enough to be neglected. This also means that the source resistance RS may be a maximum of about 2.8 kohms.

To avoid the power amplifier's input impedance also attenuating the signal too much, one can require that the power amplifier input resistance RL is not much lower than 10 times the maximum RS, i.e. approximately 30 kohm.

Modeling the cable is not an easy task, but the easiest thing to do is to look at the capacitance per unit length: pF/m. It seems that typical, this is about C = 50 pF/m. A quick calculation with our RS about 3 kohm (with a high RL, a lower RL will reduce the resistance), will give us a cutoff frequency of approx.:

f1 = 1/(2πRSC) = 1 MHz

This is well above the audio spectrum and is in large contrast to claims that passive preamplifiers limit high-frequency reproduction and/or reduce the dynamics of the signal. Even with a 10 meter cable, I would assume that cable capacitance is not a problem if your source have a reasonable output impedance. It is of course true that the cutoff frequency is volume setting position dependant, but we are talking of very, very high frequencies far above audio frequencies. However, if RL is to small compared to RS, the signal may be too much attenuated.

A practical preamplifier

The figure below shows the simplified schematic diagram for my own passive preamplifier (one channel).


An old-fashioned solution with an input selector and a tape monitor function is used. The input called Record is connected to my Streamer. The volume potentiometer has a value of 10 kohm. The input impedance of my power amplifier is about 33 kohm, but this has not been a problem. Neither has lack of amplification been a problem.

Below are pictures of the preamplifier.

  


Schematic

The complete schematic of the amplifier is shown in the figure below.


The phono connectors J1-3 is for the source inputs: Phono, Tuner and CD, while J4 is for the Record input. The resistors R1-R4 is isolating the input grounds from the output ground. The selector SW1 choose between the source inputs. The outputs from this is fed to the source/monitor switch SW2 and to the selectors J7 and J8. These are used to choose between the output from the volume potentiometer RV1 or from the output of switch SW1. The switch SW2 selects between the sources from SW1 and the Rec input. The midpoint of this switch has a mute function (the output is grounded). From SW2 the signals are fed to the volume potentiometer and further to the preamplifier output connector J6. Please observe that it is possible also to use the output connector J5 as a parallel preamplifier output.

Printed Circui Board

The layout of the complete schematic of the amplifier is shown in the figure below. In the final amplifier the volume control was changed from Elma RK27 to a potentiometer called DACT with better performance.


With 3D in KiCad, the printed circuit board looks like this:



Bill of Material

R1-R4 10 ohm (not critical) 0.6 W 1% metal film resistor
RV1 10 kohm Potentiometer Elma RK27 (Replaced by DACT Potentiometer in final amplifier build)
SW1-SW2 E-Switch 1004P6T1B4M7RE
J1-J6 RCA Jack RCJ-22 Same Sky
J7-J8 Connector Pin Header P 2.54 mm

Please notice:
This project description is for non-commercial use, only. Using this document on a site and charging a fee for download is vialation of non-commercial use and prone to demand for payment. So, for commercial use, contact me for agreement of terms. This page, however, can be downloaded for own use, and linked to, not violating term of non-commercial use.

 
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Knut Harald Nygaard