Attenuator (electronics)
An attenuator is an electronic device that reduces the power of a signal without appreciably distorting its waveform.
An attenuator is effectively the opposite of an amplifier, though the two work by different methods. While an amplifier provides gain, an attenuator provides loss, or gain less than 1.
Construction and usage
Attenuators are usually passive devices made from simple voltage divider networks. Switching between different resistances forms adjustable stepped attenuators and continuously adjustable ones using potentiometers. For higher frequencies precisely matched low VSWR resistance networks are used.Fixed attenuators in circuits are used to lower voltage, dissipate power, and to improve impedance matching. In measuring signals, attenuator pads or adapters are used to lower the amplitude of the signal a known amount to enable measurements, or to protect the measuring device from signal levels that might damage it. Attenuators are also used to 'match' impedance by lowering apparent SWR.
Attenuator circuits
Basic circuits used in attenuators are pi pads and T pads. These may be required to be balanced or unbalanced networks depending on whether the line geometry with which they are to be used is balanced or unbalanced. For instance, attenuators used with coaxial lines would be the unbalanced form while attenuators for use with twisted pair are required to be the balanced form.Four fundamental attenuator circuit diagrams are given in the figures on the left. Since an attenuator circuit consists solely of passive resistor elements, it is both linear and reciprocal. If the circuit is also made symmetrical, then the input and output ports are not distinguished, but by convention the left and right sides of the circuits are referred to as input and output, respectively.
Various tables and calculators are available that provide a means of determining the appropriate resistor values for achieving particular loss values. One of the earliest was published by the NAB in 1960 for losses ranging from 1/2 to 40 dB, for use in 600 ohm circuits.
Attenuator characteristics
Key specifications for attenuators are:- Attenuation expressed in decibels of relative power. A 3 dB pad reduces power to one half, 6 dB to one fourth, 10 dB to one tenth, 20 dB to one hundredth, 30 dB to one thousandth and so on. For voltage, you double the dBs so for example 6 dB is half in voltage.
- Nominal impedance, for example 50 ohm
- Frequency bandwidth, for example DC-18 GHz
- Power dissipation depends on mass and surface area of resistance material as well as possible additional cooling fins.
- SWR is the standing wave ratio for input and output ports
- Accuracy
- Repeatability
RF attenuators
Important characteristics are:
- accuracy,
- low SWR,
- flat frequency-response and
- repeatability.
Audio attenuators
A line-level attenuator in the preamp or a power attenuator after the power amplifier uses electrical resistance to reduce the amplitude of the signal that reaches the speaker, reducing the volume of the output. A line-level attenuator has lower power handling, such as a 1/2-watt potentiometer or voltage divider and controls preamp level signals, whereas a power attenuator has higher power handling capability, such as 10 watts or more, and is used between the power amplifier and the speaker.- Power attenuator
- Guitar amplifier
Component values for resistive pads and attenuators
- All impedance, currents, voltages and two-port parameters will be assumed to be purely real. For practical applications, this assumption is often close enough.
- The pad is designed for a particular load impedance, ZLoad, and a particular source impedance, Zs.
- *The impedance seen looking into the input port will be ZS if the output port is terminated by ZLoad.
- *The impedance seen looking into the output port will be ZLoad if the input port is terminated by ZS.
Terms used
- Pad will include pi-pad, T-pad, L-pad, attenuator, and two-port.
- Two-port will include pi-pad, T-pad, L-pad, attenuator, and two-port.
- Input port will mean the input port of the two-port.
- Output port will mean the output port of the two-port.
- Symmetric means a case where the source and load have equal impedance.
- Loss means the ratio of power entering the input port of the pad divided by the power absorbed by the load.
- Insertion Loss means the ratio of power that would be delivered to the load if the load were directly connected to the source divided by the power absorbed by the load when connected through the pad.
Symbols used
- ZS = the output impedance of the source.
- ZLoad = the input impedance of the load.
- Zin = the impedance seen looking into the input port when ZLoad is connected to the output port. Zin is a function of the load impedance.
- Zout = the impedance seen looking into the output port when Zs is connected to the input port. Zout is a function of the source impedance.
- Vs = source open circuit or unloaded voltage.
- Vin = voltage applied to the input port by the source.
- Vout = voltage applied to the load by the output port.
- Iin = current entering the input port from the source.
- Iout = current entering the load from the output port.
- Pin = Vin Iin = power entering the input port from the source.
- Pout = Vout Iout = power absorbed by the load from the output port.
- Pdirect = the power that would be absorbed by the load if the load were connected directly to the source.
- Lpad = 10 log10 always. And if Zs = ZLoad then Lpad = 20 log10 also. Note, as defined, Loss ≥ 0 dB
- Linsertion = 10 log10. And if Zs = ZLoad then Linsertion = Lpad.
- Loss ≡ Lpad. Loss is defined to be Lpad.
Symmetric T pad resistor calculation
Symmetric pi pad resistor calculation
L-Pad for impedance matching resistor calculation
If a source and load are both resistive then a resistive L-pad can be used to match them to each other. As shown, either side of the L-pad can be the source or load, but the Z1 side must be the side with the higher impedance.Large positive numbers means loss is large. The loss is a monotonic function of the impedance ratio. Higher ratios require higher loss.
Converting T-pad to pi-pad
This is the Y-Δ transformConverting pi-pad to T-pad
This is the Δ-Y transformConversion between two-ports and pads
T-pad to impedance parameters
Impedance parameters to T-pad
Impedance parameters to pi-pad
Pi-pad to admittance parameters
Admittance parameters to pi-pad
General case, determining impedance parameters from requirements
Because the pad is entirely made from resistors, it must have a certain minimum loss to match source and load if they are not equal.The minimum loss is given by
Although a passive matching two-port can have less loss, if it does it will not be convertible to a resistive attenuator pad.
Once these parameters have been determined, they can be implemented as a T or pi pad as discussed above.