refractioncat
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I'm planning to build some VPR/EPA absorbers in an attempt to improve seat-to-seat consistency in my living room in the 57-300Hz range, and I have an opportunity to do some comparisons along the lines of the Trapping Traps experiment. I'd like to get measurement data out of it that is as high-quality as possible.
I have 6 panels (120x60cm x 50mm) of Caruso Iso-Bond WLG035, 3 steel sheets of different thicknesses (100x50cm x 0.6, 0.8 & 1.0mm), and a few other supplies like some melamine foam and PET house insulation (very similar to fluffly fiberglass but less irritating).
The room I have available for this experiment is roughly 350cm long, 320cm wide, and 240cm high. From the door, the left side has a closet and the right side has a large window. There is some furniture present that I cannot realistically remove from the room.
For the hardware I'd be using a Wharfedale Diamond 12.1 speaker, Fosi ZA3 amplifier, and UMIK-1 microphone, all connected to a laptop. This means that realistically I'm limited to frequencies above 50 Hz, but this is fine because the range I'm mostly interested in is 57 Hz upwards.
I am considering two different setups for the experiment:
In the modal setup, I would be essentially copying Trapping Traps with a worse room with a fair amount of pre-existing absorption, and smaller absorbers (0.7m^2 instead of 2m^2).
The speaker would be on the floor level at position S. The microphone would be near the ceiling at position M. The absorbers could be placed straddling a corner at A1, flat in a corner at A2, or flat away from the corner at A3 or A4. The room would be measured empty, and with each absorber configuration, and the decay times can be evaluated, insofar as any meaningful difference can be detected. With some configurations I'd be able to use absorbers stacked or side-by-side to increase the area to 1.4m^2 or 2.1m^2.
Because of the issues with the modal setup, I've thought of an alternative using SBIR to isolate frequencies of interest. The speaker would be placed along the wall at varying distances in area S, the absorber would be at A to treat the null caused from the wall reflection, and the microphone would be at either M1 or M2. This requires separate measurements for each distance with each absorber (and the control condition), and then the frequency of the nulls and their depth could be evaluated. The frequency of interest can be controlled fairly precisely by the distance from the wall, and apart from the frequencies where the ceiling/sidewall reflection would interfere, it seems like at least the relative performance differences between absorbers could give some useful information.
My plan would be to mark the test positions with tape on the baseboard, and move the speaker between positions while keeping the absorber setup constant for each absorber. To check the reliability of this process, I'd take multiple control measurements where I move the speaker between the different positions to see how consistent the cancellation frequencies and depths are between different attempts to place the speaker in the exact same positions. The microphone would stay stationary through the measurement session; if I have to move the microphone, or it moves by accident, I'd treat that as a separate session, retake the control measurements, and distinguish between the sessions in the results.
The M2 mic position is more convenient and less likely to have to move between measurements. The M1 position seems slightly better geometrically, and allows moving the microphone outside the room if a greater speaker-mic distance is needed for lower frequencies and the reflections from the hallway don't make things too messy.
I can address the sidewall reflection somewhat by placing something absorptive in the way, but I don't have a practical way to deal with the ceiling reflection meaning that around 50ish Hz (if I calculated it right) would be inevitably confounded.
---
The absorber configurations of interest are:
Pure porous absorbers:
Iso-Bond (120x60cm): 5, 10, 15, 20, 25, 30cm
Melamine foam (100x50cm): 5, 10, 15, 20cm
VPRs (with Iso-Bond as the damping material, each with 0.6, 0.8 & 1.0mm plates):
5cm + steel
10cm + steel
15cm + steel
EPAs (steel of each thickness sandwiched between Iso-Bond):
5cm + steel + 5cm
10cm + steel + 5cm
5cm + steel + 10cm
In addition, I'm interested in trying out a couple of experimental solutions to see whether they work:
Bean bag chair bass trap:
Around 100x100x80cm, filled with polyester; turned out to be a lousy chair but maybe it could be an aesthetically inconspicuous superchunk.
Multi-plate VPR/EPA:
Stacking the thinner steel plates to see whether they can achieve a better performance in low frequencies due to having the pistonic effect of a thicker plate but the lower bending stiffness of a thinner one. I can use a very large mousepad (roughly 40x90cm) to decouple the plates a bit if needed.
Edge-on absorption:
Placing Iso-Bond absorbers on the wall in line with the sound waves, instead of face-on, to see what happens; or in other words, 120x10cm and 120x20cm panels with 60cm thickness and different airflow resistance behaviours due to the material's anisotropy.
---
To get the necessary disclaimer out of the way, I've read+watched my Sauro and understand that this is very much a "I changed something and then something happened" experiment. The 120x60cm VPR is a particularly convenient size for people to make because, at least in the UK, 100x50cm steels are easily available on e.g. ebay, and I haven't found much data beyond "these are the before and after measurements from my room", so I figured I'd try contributing something back to the commons.
I'd appreciate any feedback/criticism about the experiment design and setup, and opinions on whether I should go with the modal setup or the SBIR setup, or even both. Any ideas on additional tests that you'd like to see performed, that can be performed with the supplies, gear and space I have, are also welcome.
I have 6 panels (120x60cm x 50mm) of Caruso Iso-Bond WLG035, 3 steel sheets of different thicknesses (100x50cm x 0.6, 0.8 & 1.0mm), and a few other supplies like some melamine foam and PET house insulation (very similar to fluffly fiberglass but less irritating).
The room I have available for this experiment is roughly 350cm long, 320cm wide, and 240cm high. From the door, the left side has a closet and the right side has a large window. There is some furniture present that I cannot realistically remove from the room.
For the hardware I'd be using a Wharfedale Diamond 12.1 speaker, Fosi ZA3 amplifier, and UMIK-1 microphone, all connected to a laptop. This means that realistically I'm limited to frequencies above 50 Hz, but this is fine because the range I'm mostly interested in is 57 Hz upwards.
I am considering two different setups for the experiment:
In the modal setup, I would be essentially copying Trapping Traps with a worse room with a fair amount of pre-existing absorption, and smaller absorbers (0.7m^2 instead of 2m^2).
The speaker would be on the floor level at position S. The microphone would be near the ceiling at position M. The absorbers could be placed straddling a corner at A1, flat in a corner at A2, or flat away from the corner at A3 or A4. The room would be measured empty, and with each absorber configuration, and the decay times can be evaluated, insofar as any meaningful difference can be detected. With some configurations I'd be able to use absorbers stacked or side-by-side to increase the area to 1.4m^2 or 2.1m^2.
Because of the issues with the modal setup, I've thought of an alternative using SBIR to isolate frequencies of interest. The speaker would be placed along the wall at varying distances in area S, the absorber would be at A to treat the null caused from the wall reflection, and the microphone would be at either M1 or M2. This requires separate measurements for each distance with each absorber (and the control condition), and then the frequency of the nulls and their depth could be evaluated. The frequency of interest can be controlled fairly precisely by the distance from the wall, and apart from the frequencies where the ceiling/sidewall reflection would interfere, it seems like at least the relative performance differences between absorbers could give some useful information.
My plan would be to mark the test positions with tape on the baseboard, and move the speaker between positions while keeping the absorber setup constant for each absorber. To check the reliability of this process, I'd take multiple control measurements where I move the speaker between the different positions to see how consistent the cancellation frequencies and depths are between different attempts to place the speaker in the exact same positions. The microphone would stay stationary through the measurement session; if I have to move the microphone, or it moves by accident, I'd treat that as a separate session, retake the control measurements, and distinguish between the sessions in the results.
The M2 mic position is more convenient and less likely to have to move between measurements. The M1 position seems slightly better geometrically, and allows moving the microphone outside the room if a greater speaker-mic distance is needed for lower frequencies and the reflections from the hallway don't make things too messy.
I can address the sidewall reflection somewhat by placing something absorptive in the way, but I don't have a practical way to deal with the ceiling reflection meaning that around 50ish Hz (if I calculated it right) would be inevitably confounded.
---
The absorber configurations of interest are:
Pure porous absorbers:
Iso-Bond (120x60cm): 5, 10, 15, 20, 25, 30cm
Melamine foam (100x50cm): 5, 10, 15, 20cm
VPRs (with Iso-Bond as the damping material, each with 0.6, 0.8 & 1.0mm plates):
5cm + steel
10cm + steel
15cm + steel
EPAs (steel of each thickness sandwiched between Iso-Bond):
5cm + steel + 5cm
10cm + steel + 5cm
5cm + steel + 10cm
In addition, I'm interested in trying out a couple of experimental solutions to see whether they work:
Bean bag chair bass trap:
Around 100x100x80cm, filled with polyester; turned out to be a lousy chair but maybe it could be an aesthetically inconspicuous superchunk.
Multi-plate VPR/EPA:
Stacking the thinner steel plates to see whether they can achieve a better performance in low frequencies due to having the pistonic effect of a thicker plate but the lower bending stiffness of a thinner one. I can use a very large mousepad (roughly 40x90cm) to decouple the plates a bit if needed.
Edge-on absorption:
Placing Iso-Bond absorbers on the wall in line with the sound waves, instead of face-on, to see what happens; or in other words, 120x10cm and 120x20cm panels with 60cm thickness and different airflow resistance behaviours due to the material's anisotropy.
---
To get the necessary disclaimer out of the way, I've read+watched my Sauro and understand that this is very much a "I changed something and then something happened" experiment. The 120x60cm VPR is a particularly convenient size for people to make because, at least in the UK, 100x50cm steels are easily available on e.g. ebay, and I haven't found much data beyond "these are the before and after measurements from my room", so I figured I'd try contributing something back to the commons.
I'd appreciate any feedback/criticism about the experiment design and setup, and opinions on whether I should go with the modal setup or the SBIR setup, or even both. Any ideas on additional tests that you'd like to see performed, that can be performed with the supplies, gear and space I have, are also welcome.
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