THE PHYSICS OF QUIET / 05

Insertion Loss in Audio Systems

How a Matrix Boundary reduces the unwanted high-frequency energy that reaches a protected part of an audio system.

An audio system is a connected electrical environment. Unwanted high-frequency energy can travel along power, grounding, chassis and interconnect paths, reaching parts of the system we would rather keep quiet. Insertion Loss gives us a way to describe how much of that energy is reduced as it passes through a treatment point.

Where Return Loss describes what comes back from a boundary, Insertion Loss describes what continues beyond it. This page follows the energy that attempts to cross a Matrix Boundary and enter a protected area.

A note on the model: the animation is an illustrative high-frequency wave model. It explains a mechanism and a direction of change; it is not a measured response of a particular Quiescent product or a prediction for every installation.

Waves rolling onto a shallow beach with a calmer lagoon behind as an analogy to insertion loss in audio systems

The shallow beach is the boundary

Reading the lagoon image

The image is deliberately not a harbour wall. A hard wall sends a wave back and is useful when explaining reflection. A shallow beach gives an incoming wave a long, changing route over which it can lose energy. The lagoon beyond the beach is calmer because less of the incoming wave reaches it.

  • The sea represents unwanted high-frequency energy approaching the system.
  • The shallow beach represents the Matrix Boundary: a treatment point in that energy’s route.
  • The lagoon represents the protected part of the system.
  • The energy lost across the beach represents Insertion Loss: a reduction in the unwanted energy able to cross into the protected area.

Insertion Loss is therefore about transmission. At 0 dB, the illustrative incoming wave crosses the Matrix Boundary without attenuation. As Insertion Loss increases, less unwanted energy reaches the protected area.

Return Loss and Insertion Loss are complementary, not interchangeable. Return Loss describes energy reflected back at a boundary. Insertion Loss describes energy transmitted through it. In the animation below, Return Loss is held at 20 dB so the small reflected wave stays constant while the transmitted wave changes.

Illustrative Matrix Insertion Loss
Incident wave Reflected wave · fixed 20 dB Return Loss Transmitted wave
Matrix Insertion Loss
Transmitted power
Transmitted amplitude
Interactive illustration of a wave crossing a Matrix Boundary into a protected area. Matrix Return Loss is fixed at 20 dB. Select a Matrix Insertion Loss to update the transmitted wave.

How to read the graphic: the blue incident wave approaches from the external field. The narrow green reflected trace is deliberately held constant at 20 dB Return Loss. Beyond the Matrix Boundary, the dark transmitted wave shows the energy entering the protected area. Changing Insertion Loss changes that transmitted wave and its two readouts only.

What the control changes

The control changes only the illustrative Matrix Insertion Loss. The incident wave remains the same. Matrix Return Loss remains fixed at 20 dB. This makes the relationship clear: the changing quantity is the energy that crosses the boundary into the protected area.

Insertion Loss is stated in decibels, so the change is logarithmic rather than linear. A 3 dB Insertion Loss leaves about half the illustrative power to continue. At 10 dB, one tenth remains. At 20 dB, one hundredth remains. The animation shows both transmitted power and transmitted amplitude because they describe different aspects of the same wave.

At 0 dB, the transmitted wave continues at the same illustrative amplitude as the incident wave. As the selected value rises, the transmitted trace becomes progressively smaller. At 30 dB, the model leaves only 0.1% of the incident power and about 3.2% of the incident amplitude beyond the Matrix Boundary.

Begin at 0 dB

At 0 dB there is no illustrative Insertion Loss. The incident wave crosses the Matrix Boundary and enters the protected area at full amplitude. This is the useful starting comparison, not the desired outcome.

Increase Insertion Loss

Move through 3, 6, 10, 20 and 30 dB. The incident wave and the small fixed reflection do not change. Watch only the transmitted wave beyond the Matrix Boundary become smaller.

Read power and amplitude

The component reports both ratios. At 10 dB, 10% of the illustrative power crosses the boundary, while the transmitted voltage-amplitude ratio is about 31.6%.

A simple comparison

  1. Begin at 0 dB. The transmitted wave entering the protected area has the same illustrative amplitude as the incident wave.
  2. Select 3 dB. About half of the illustrative incident power now crosses the Matrix Boundary.
  3. Select 10 dB. One tenth of the illustrative power remains, and the transmitted amplitude is about 31.6%.
  4. Compare 20 dB and 30 dB. The protected-area trace approaches the baseline as the transmitted energy falls to 1% and then 0.1% of the starting power.
  5. Notice that the reflected trace does not change. Return Loss is intentionally fixed here so the comparison isolates Insertion Loss.

From the beach to a measurement

The lagoon is an analogy, not a literal electrical model. In engineering terms, Insertion Loss compares the power that arrives at a treatment point with the power that emerges beyond it. The central question is simple: how much of the unwanted high-frequency energy is allowed to continue into the part of the system we are trying to protect?

Insertion Loss describes what crosses

For this illustration, Insertion Loss compares incident power with the power transmitted beyond the Matrix Boundary, expressed in decibels:

Insertion Loss = −10 log10(transmitted power ÷ incident power)

Higher Insertion Loss therefore means less transmitted power. The amplitude ratio is the square root of the power ratio, so it changes at half the decibel rate. The table uses the same relationship as the component above.

Illustrative Insertion Loss Transmitted power Transmitted amplitude
0 dB — no loss 100% 100%
3 dB About 50% About 71%
6 dB About 25% About 50%
10 dB 10% About 32%
20 dB 1% 10%
30 dB 0.1% About 3.2%

Exact behaviour depends on the device, cable and installation

Higher Insertion Loss means less unwanted high-frequency energy reaches the protected area

The graph shows a design objective: little or no attenuation through the audio band, with increasing attenuation of unwanted high-frequency energy. It explains the intended direction of control, rather than presenting a measured response of a particular Quiescent product.

Illustrative plot of ideal insertion loss against frequency for audio systems

This frequency illustration describes a design objective for controlling unwanted high-frequency energy. It is explanatory rather than a published measurement of a particular Quiescent product.

Why the protected area matters

At conventional audio frequencies, many system connections can often be treated as straightforward circuit paths. As frequency rises, the electrical route becomes more significant. Cable geometry, connector interfaces, chassis structures, component parasitics and the paths shared by power and grounding can all influence where unwanted energy travels.

That does not mean every audio connection behaves as an ideal RF transmission line, or that one Insertion Loss value explains an entire system. It means that high-frequency energy needs to be considered as movement through a connected environment. The protected area in the illustration represents a part of that environment in which we want less unwanted energy to arrive.

Insertion Loss in this context is not a claim that the wanted audio signal should be attenuated. The design question is how to reduce unwanted high-frequency energy while preserving the intended audio-band behaviour of the system.

Insertion Loss and Return Loss work together

A Matrix Boundary has two related jobs. It should reduce the unwanted energy that passes into the protected area; that is the Insertion Loss view. It should also avoid sending a large part of that energy back into the wider system; that is the Return Loss view.

This page holds Matrix Return Loss at 20 dB to concentrate on transmission. The companion Return Loss in Audio Systems page holds the transmission question aside and makes the reflected field visible. Together, the two models describe a more considered route for unwanted energy than a simple hard barrier.

Quiescent’s interest is not to impose a house sound or remove musical energy. It is to reduce uncontrolled high-frequency conditions that can complicate the electrical environment in which the system is trying to work.

Why less unwanted energy can matter to music

Music asks an audio system to preserve relationships of level, timing and harmonic structure as they change moment by moment. Reducing the unwanted energy allowed into a sensitive part of the system is intended to create a quieter, more stable operating condition in which that task is less impeded.

This is not a guarantee of one sonic signature. In a resolving system, the practical signs may instead be greater image stability, cleaner leading edges, more distinct low-level detail and less congestion when the music becomes complex. The related Tracking Error in Audio Systems page makes that relationship visible as a conceptual model.

Explore further

Matrix boundaries

Return Loss

How a controlled boundary reduces the energy reflected back into the system.

Explore Return Loss

System application

Subsystem Protection

How two Matrix boundaries can define a quieter environment around a sensitive part of a system.

Explore Audio Subsystem Protection

Signal behaviour

Tracking Error

How a changing disturbance environment can make it harder for a system to follow the musical signal precisely.

Explore Tracking Error

Technical notes and further reading

This page uses a conceptual high-frequency illustration. Insertion Loss is used here in its engineering sense: the reduction in transmitted power through a path or component, expressed in decibels. The references below explain the underlying terminology and high-frequency behaviour; they do not constitute independent performance verification of Quiescent products.