Description: A VU-meter is a common instrument typically found on audio Hi-Fi amplifiers, designed to display the instantaneous power delivered to the speakers. It is usually connected at the amplifier's output, in parallel with the speaker. The term "VU" stands for Volume Unit, with 0VU corresponding to +4dBm or 1.23RMS across a 600-ohm load. 0VU is often referred to as "0dB," and volume units are rarely utilized. In consumer electronics amplifiers, this standard is seldom met, and the meters generally indicate the amplifier's power without referencing any physical unit. The primary interest is in the power output to the speakers, rather than volume units. Thus, a meter providing a reading between zero and the maximum output power is generally sufficient. Audio volume is typically expressed on a logarithmic scale, reflecting the logarithmic nature of human auditory perception. Direct power readings in Watts may not effectively represent perceived volume. For instance, a few millivolts on an 8-ohm speaker are clearly audible. At low volume, speaker voltage may only reach a few hundred millivolts (milliwatts), while at medium volume, it rises to a few volts (around one Watt), and only at high volumes does the amplifier output its full power. Non-professional audio amplifiers often feature simple and ineffective VU-meters. For example, a circuit diagram found in an 80WRMS stereo set includes a diode rectifier (a voltage doubler consisting of C1, D1, and D2), a filter capacitor (C2), and a microammeter (M1). The full scale is adjustable via R1 to match the amplifier's maximum power output. However, this simple circuit results in a reading proportional to the peak output voltage, which is low and only increases significantly at high volumes, leading to meters that rarely move. Additionally, the use of a voltage doubler is questionable, as the speaker voltage is already sufficiently high, and the silicon diodes used have a forward voltage drop of about 0.6V, whereas germanium or Schottky diodes would have a lower drop. The doubler also has twice the forward voltage drop of a single diode, preventing small signals from being registered. Consequently, any signal below 1.2V peak will not move the meter, rendering this design ineffective. For meaningful readings, a logarithmic meter is necessary to measure both low and high power levels effectively. Professional or high-end amplifiers feature high-quality meters with logarithmic converters built from multiple op-amps and various components. However, a simple and passive logarithmic VU-meter can be constructed with minimal parts. Linear meters, like the previously described one, can also be converted. The fundamental concept involves utilizing the logarithmic characteristics of diodes to achieve a logarithmic response in an electromechanical microammeter. The circuit is straightforward and based on a standard 200µA microammeter, which is commonly used for such applications. The internal resistance is not critical and typically ranges between 500 ohms and 1k ohms. This circuit is designed for amplifiers capable of 80WRMS driving an 8-ohm load but can be easily adapted for different power levels or impedances. Similar power levels require no modifications, while significantly higher or lower levels necessitate adjustments to R4, and possibly R2 and R3. The AC signal across the speaker is first rectified by diode D1, which should be a germanium diode.
The VU-meter circuit design incorporates several essential components to ensure accurate power level readings. The primary elements include a rectifier, which converts the AC signal from the speaker into a DC signal, and a logarithmic scaling mechanism that adjusts the output to reflect perceived volume levels accurately. The rectifier, typically a germanium diode, is chosen for its low forward voltage drop, which allows for the detection of smaller signals that would otherwise be ignored by silicon diodes. Following rectification, a filter capacitor smooths the output to provide a stable DC voltage to the microammeter.
The microammeter, which serves as the display element, is calibrated to represent the logarithmic scale of the audio signal. To achieve this, the circuit employs a logarithmic response characteristic of the diodes, which allows for a more accurate representation of perceived loudness across a wide range of input levels. Resistors R1, R2, R3, and R4 play a crucial role in setting the scale and sensitivity of the meter. R1 adjusts the full-scale reading to match the amplifier's maximum output, while R2 and R3 may be altered to fine-tune the response for different power levels.
So a meter that gives a reading between zero and the maximum power output is fine enough (at least, for me). The audio volume is often expressed using a logarithmic scale because the feeling of sound intensity we get from our ears is also logarithmic and a direct power reading in Watts would not be very representative of the perceived volume.
So the amplifier has two nice meters that almost never move. Furthermore, the use of a voltage doubler is very surprising (and a bad idea), first because the voltage on the speakers is already high enough and there is no need to double, than because it`s composed by silicon diodes that have a forward voltage drop of about 0. 6V while germanium or Schottky diodes would drop much less, and finally because a doubler has twice the forward voltage drop of a single diode preventing small signals to go through.
In this configuration, any signal lower than 1. 2Vpeak has no chance of moving the meter. So this diagram has a big red cross: it`s a bad idea, don`t use it. In order to have meaningful readings, the meter should be logarithmic, allowing measures of low and high power levels without the problems mentioned above. Professional or high-end amplifiers have good meters with logarithmic converters built with many op-amps and lots of parts, but there is a way to build a simple and passive logarithmic VU-meter with only a few parts.
Similar power levels requires no modification, for much higher or lower levels, R4 must be modified and maybe also R2 and R3. First the AC signal across the speaker is rectified by diode D1. D1 should be a germa
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