Understanding sound transmission loss (TL)

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Discussion Overview

The discussion revolves around the calculation of sound transmission loss (TL) when a sound wave in air encounters a wall. Participants explore the implications of TL on the power of reflected sound waves, examining derivations and assumptions related to the equations governing these phenomena.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant presents a formula for TL and derives an equation for the diminished power of the reflected wave, seeking validation of their reasoning.
  • Another participant suggests that the model assumes the wall behaves like a mismatched transmission line and emphasizes the need to define W2 as the sound power entering the wall rather than the power radiated on the far side.
  • Some participants propose separately calculating losses due to absorption and transmission, indicating that the absorption coefficient of the wall material is relevant to the discussion.
  • There is a mention of conservation of energy in the context of the relationship between incident, transmitted, absorbed, and reflected power.
  • A later reply questions the initial assumption of zero reflection in the first equation and suggests a more complete formula that includes the reflection coefficient.

Areas of Agreement / Disagreement

Participants express differing views on the assumptions made in the derivation of equations related to TL and reflected power. No consensus is reached on the validity of the initial derivation or the implications of the conservation of energy in this context.

Contextual Notes

Some assumptions regarding the definitions of W2 and the treatment of reflection and absorption are not fully resolved. The discussion highlights the complexity of applying decibel calculations in this context.

Pete_L
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In considering a sound wave (in air) incident on a wall, the transmission loss (TL) is calculated by the equation

TL (dB) = 10*Log (W1/W2)
where
W1 = sound power incident on wall
W2 = sound power transmitted through wall

Based on this understanding of TL, I wish to determine the extent to which TL diminishes sound power of the reflected sound wave. Understanding that W1/W2 is the ratio of sound powers, I calculated

Lt (dB) = 10*Log [ 1- (W2/W1)]
where
Lt = the extent to which power of the reflected wave is diminished relative to that of the incident wave due to some of the power transmitted through the wall

This might become part of an article that I hope will be published. As I am not a professional, I just wanted to check that my derivation from the standard equation for transmission loss is correct. So thanks if someone who is knowledgeable concerning acoustics can confirm that this is correct or not.

-Pete
 
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To make this easier to respond to, here is how I derived the equation for Lt.
Consider the fraction below,

[(W1/W2) -1] / (W1/W2)

If for example W1/W2 equals 10, this means 10 parts incident sound power to 1 part transmitted power. In the numerator, 10 minus 1 equals 9. The denominator is the original ratio of 10 without subtracting the 1 part of transmitted sound power. Thus,

10*log [((W1/W2) - 1 ) / (W1/W2)] = 10*log 0.9 = -0.46 dB

This tells me that power in the reflected wave with respect to power of the incident wave has been diminished by about 0.5 dB as a result of some of the energy transmitted through the wall.

Simplifying the fraction,

(W1/W2) -1 = (W1 - W2) / W2

[(W1- W2) / W2] * 1/(W1/W2) = (W1- W2)/ W1

(W1 - W2)/ W1 = 1 - (W2 / W1)
Then
Lt = 10*Log [1- (W2 / W1)]

Please tell me if this is a false line of reasoning, or not. Thank you in advance if anyone can.
-P
 
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I think the simple model for reflection you are using assumes that the wall is acting like a piece of mismatched transmission line.
But W2 will be affected by the heat losses in the wall. You would need to define W2 as the sound power entering the wall rather than the sound power radiated on the far side.
An analogue might be the power reflected from a mismatched attenuator in a transmission line.
 
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tech99 said:
I think the simple model for reflection you are using assumes that the wall is acting like a piece of mismatched transmission line.
But W2 will be affected by the heat losses in the wall. You would need to define W2 as the sound power entering the wall rather than the sound power radiated on the far side.
An analogue might be the power reflected from a mismatched attenuator in a transmission line.

My approach is to separately calculate loss due to absorption and transmission. I came across an equation for approximating transmission loss only. Then I also can approximate absorption knowing what the material of the wall is and knowing the absorption coefficient for that material.

But my question is- Is my method of deriving an equation for attenuated power of the reflected sound wave correct? Assume that I have a correct value of W2, whatever that is.

-P
 
Pete_L said:
My approach is to separately calculate loss due to absorption and transmission. I came across an equation for approximating transmission loss only. Then I also can approximate absorption knowing what the material of the wall is and knowing the absorption coefficient for that material.

But my question is- Is my method of deriving an equation for attenuated power of the reflected sound wave correct? Assume that I have a correct value of W2, whatever that is.

-P
Yes, correct I believe.
 
Isnt all this just restating conservation of energy? Eg...

Incident power - transmitted power - absorbed power - reflected power = 0
 
tech99 said:
Yes, correct I believe.

Thank you, I'm not always as rigorous as I should be in solving a problem.
-P
 
CWatters said:
Isnt all this just restating conservation of energy? Eg...

Incident power - transmitted power - absorbed power - reflected power = 0

What I need to solve is dB of loss, or reflected power relative to incident power in dB, without regard to the amount of acoustic power involved. So regardless of any particular incident power, the reflected power is reduced by some dB amount.
 
CWatters said:
Isnt all this just restating conservation of energy? Eg...

Incident power - transmitted power - absorbed power - reflected power = 0
Yes, but I think the OP question related to the use of decibels, which can be tricky when subtraction or addition are involved.
 
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Pete_L said:
In considering a sound wave (in air) incident on a wall, the transmission loss (TL) is calculated by the equation

TL (dB) = 10*Log (W1/W2)
where
W1 = sound power incident on wall
W2 = sound power transmitted through wall

Based on this understanding of TL, I wish to determine the extent to which TL diminishes sound power of the reflected sound wave. Understanding that W1/W2 is the ratio of sound powers, I calculated
Your first equation assumes zero reflection. As you assume zero reflection, it seems odd to use this formula to find something about reflected wave.
The complete formula should be
## L_t=10 log \frac{W1(1-R)}{W2} ##
where R is the coefficient of reflection (intensity) at the interface.
The intensity of the reflected wave depends on the impedance mismatch at the interface. You want to study deviations from Frenel's equations predictions due to absorption in the second medium?
 
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