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Midrange compression driver development |
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JulianDA
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Topic: Midrange compression driver developmentPosted: 17 April 2024 at 10:49pm |
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Our latest project is is the development and construction of a 3-way fully hornloaded midtop. The goal is to reproduce frequencies from 200/250Hz and upwards with high sensitivity and a controlled directivity of 60 by 40 degrees. At the moment our low-mid driver is the 18S 12ND610 which will cover 200-800Hz. The Midrange is a B&C 6NSM51 which should be covering 800-3500Hz. The HF Driver is not specified at the moment. All we know so far is that it should be a 1" CD, but we are still searching for the right one (Any recommendations?).
In this thread i want to talk about the midrange driver and horn. In my opinion it is the heart of the whole project and also the hardest part to get right. The plan is to design a midrange compression driver with the 6NSM51, which really just means to design a phaseplug with a pretty high compression-ratio analogous to your typical hf compression drivers. JBL did the same with their CMCDs (Cone Midrange Compression Drivers) as you can see in this Tech-Note: https://jblpro.com/en/site_elements/tech-note-cone-midrange-compression-drivers-cmcd I started this whole journey by reading and trying to understand the following paper from Mark Dodd and Jack Oclee-Brown: https://www.researchgate.net/publication/292662389_New_Methodology_for_the_Acoustic_Design_of_Compression_Driver_Phase_Plugs_with_Concentric_Annular_Channels The paper describes a way of generating a concentric phaseplug geometry which supresses the establishment of modes in the compression cavity by careful placement of the phaseplug channel entries. This work is for HF drivers, but the physics is the same for the midrange. So analog to Dodd and Oclee-Brown, i started with a modal analysis of the compression cavity of my -soon to be- compression driver in akabak. The following picture shows the result which is split in two halves, since i can only get akabak to show me the sound pressure over a straight line <- i managed to get two straight lines in the cavity: ![]() For a real deep dive into all this you should read the paper, or even better the full dissertation. But in short: -The four lines you can see are four resonant modes in the cavity. -Only the first two are of importance, since the driver shall only play up to max. 4kHz. -By positioning the phaseplug channel entries at the nodes of one mode, all the modes below and including that mode are supressed. with that info it was clear that i needed two channels exactly at the nodes of the second mode. I set my desired compression ratio at 7:1 (its the value JBL used and called "moderate") and began construction of the plug in CAD. The following image shows the result: ![]() The size of the channel entries is chosen according to the compression-ratio and the area of the section of membrane that "feeds" the channel. So the inner part of the membrane feeds the inner channel with a CR of 7:1 and so does the outer. The outer Channel is also curved to elongate it for pathlength correction (the difference is about 1mm. I could not get it better). Both Channels have the same expansion-rate and combine to an exit of 80mm diameter. As a whole the phaseplug starts with an area of ~20cm^2 at the channel entries and ends after a pathlength of 4,5cm with an area of ~50cm^2. Here it is. 3D-printed as three pieces that press together: ![]() ![]() And here it is mounted to our test-horn: ![]() One big problem with all of this is the simplicity of my akabak simulations. Since i can only work with TSP and the geometry of the membrane, all the stuff that can and will happen with a moving membrane (like breakup modes) is not part of my simulation. Because of this i know that my results will differ from reality. The most critical part that will differ is the position of the channel entries. But i aim to just produce more prototypes and go by trial and error from this stage on. But enough said. Here are two quick measurements i did. I also included the simulation-results. (Better measurements will follow eventually) First, here is the 6nsm51 cd on the horn (like in the last picture): Red is the measurement and blue the simulation ![]() And this is just the Driver mounted flush to the horn without any phaseplug: ![]() I think i am not to far off, but i always see a drop of 5dB starting at 2kHz that is not in the simulations. I did a lot more measurements and testing with other geometries etc. and it is a reoccuring "problem". Right now i dont have a clue why that is, so if anyone has some more insights or suggestions i would be more than happy to hear them.
PS: getting work done on this will take some time, like all of my documented projects on this site. So please dont expect fast updates ![]() |
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VECTORDJ
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Joined: 11 June 2006 Location: United States Status: Offline Points: 585 |
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Posted: 18 April 2024 at 12:58am |
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Turbosound wrote an AES Paper that talked about Cone Mid Horns....Speaker Builder Mag had a paper on Cone Mid Horns....Checkout Funktion One designs....As You found getting above 2K flat is Black Magic....Good Luck with Your Project.
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Elliot Thompson
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Joined: 02 April 2004 Location: United States Status: Offline Points: 5365 |
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Posted: 18 April 2024 at 3:17am |
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Have you measured the driver without the horn? The TS Parameters indicate an Le of 0.15 In free air you should be able to make it to around -3dB @ 6.1 kHz with a 0 dB starting point @ 1.03 kHz without the need of a Phase Plug. B&C TS Parameters in terms of 1 watt, 1 meter is lower than the advertised specifications once calculated. B&C states 100 dB sensitivity 1 watt, 1 meter whereas, calculation brings forth 94.66 dB @ 1 watt, 1 meter.
Best Regards,
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Elliot Thompson
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snowflake
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Joined: 29 December 2004 Location: Bristol Status: Offline Points: 3443 |
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Posted: 18 April 2024 at 12:47pm |
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you aren't trying to get very wide bandwidth out of this - can you not do better just using a front chamber to couple to the horn...
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fudge22
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Posted: 19 April 2024 at 12:59am |
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You have obviously spent a lot of time on the initial design and analysis of the phase plug, but then seem to have just given up and slapped it on to the back of a wooden horn, with no consideration as to how they couple. From the photos, there appears to be a relatively large discontinuity in cross sectional area from the phase plug exit and the throat of the main horn. Such discontinuities are not conducive of a smooth or optimum response. One of the benefits of using a phase plug is that it reduces the volume of the cavity between the diaphragm and the horn throat. This cavity behaves as an acoustic reactance acting as a shunt capacitance across the throat. However, it may be useful to measure the response of the driver horn combo without a phase plug to get a base line response. In his 1978 paper on phase plugs, Henricksen noted that circumferential phase plugs produced a notchy response compared to radial slit phase plugs. It might be worth experimenting with that type of design. If I remember correctly EAW used a form of radial slit phase plug to couple cone drive units to mid-range horns in some of their designs. |
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madboffin
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Posted: 20 April 2024 at 4:43pm |
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One thing to check for, as you tidy up the design, is resonances in the component parts of the phase plug i.e. the cone and the ring. They can sometimes cause suckouts and an uneven frequency response. The technical way to do this is with an accelerometer (vibration pickup) but you can do a basic check for any serious resonances by holding a finger on the relevant part while doing a frequency sweep, which will indicate if further investigation is required. |
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KDW32
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Posted: 21 April 2024 at 12:36am |
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Yes Zeus! Knowledge bomb right there.
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RoadRunnersDust
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Posted: 21 April 2024 at 7:16pm |
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What cone-plug distance have you used?
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JulianDA
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Posted: 22 April 2024 at 6:05pm |
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Do you have links to these papers if they are free to read? i could not find them. Surely i know about funktion one´s designs, but they work with a cone speaker "converted" to a ring radiator, so their designs are of little use to me.
Yes i did, but the driver was measured without any baffle. Here is the result. (red -> with horn) ![]() to me it is clear that i loose a lot of spl in the higher frequencies because of the nearly constant directivity if my horn. The driver alone measures more hf, but its directivity also becomes very narrow, while my horn disperses the sound pressure over a larger radiation angle. That is also the reason for my whole Phaseplug Design. I need more output at the higher frequencies to then disperse it over a greater angle.
No i can't since i would not get the desired directivity with the hornthroat = SD. But by reducing the throat area till its small enough for the directivity and "hf"-SPL, i get problems because of the pathlength differences and throatchamber volume.
This prototype horn was always part of the design process. I know from previous experimentation that it works really well for how simple it is constructed. Even if it doesn't look like it, the horn is also a result of numerous simulations in akabak and the construction of two other prototypes before it.
I think the photos are misleading then. The only real discontinuity is the change from a round throat to a square horn. This change is made less drastic by the triangles in the corners. But i also did a measurement without those triangles and even that had no significant effect on the response.
The last measurement of my initial post shows exactly that :)
The paper that i linked also tested radial designs and found that a properly designed circumferential plug has superior performance. The "notchy response" comes from the resonant modes inside the compression cavity. The whole aim of this design is to suppress these modes from forming by carefull placement auf the channel entries. The Notch that i measured (around 2,5kHz) is exactly that. Its the first resonant mode inside the cavity that is still excited.
Thanks for the tip! I will try if i can feel anything...but with double ear-protection...this thing is LOUD with even the slightest input :D
The distance is 2mm. Hornresp showed 0.5mm excursion at 500W input and a highpass of 800Hz. I decided that my next step will be testing slightly different phaseplugs to see if i am in the right ballpark with the position of my channels. The printer is already printing two new variants. One with both channels moved 2mm more to the outside, and one with both channels moved 2mm more to the inside. I think trial and error is the only thing i can do at this moment. |
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Elliot Thompson
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Joined: 02 April 2004 Location: United States Status: Offline Points: 5365 |
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Posted: 23 April 2024 at 2:06am |
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Measuring without a baffle is the best way as the loudspeaker's frequency response is not influence by a boundary. It appears you are having issues (major dips) within the 4 kHz - 5 kHz range once attached to the horn. If you are looking for a wider dispersion at High Frequencies, try exploring the notes from Don Keele. He was responsible for Electro-voice (Hyperbolic) and JBL (Bi-Radial) wide dispersion horns in the 1970's - 1980's. Typically either design will offer no less than 100 degree horizontal dispersion at high frequencies. Best Regards,
Edited by Elliot Thompson - 23 April 2024 at 2:09am |
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Elliot Thompson
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Timebomb
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Posted: 23 April 2024 at 4:27pm |
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I would try extending the central part of the plug into the the horn throat, try and smooth the transition. What does the impedance response look like around 2KHz?
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James Secker facebook.com/soundgearuk
James@soundgear.co.uk www.soundgear.co.uk |
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fudge22
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Posted: 23 April 2024 at 7:46pm |
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Ah! Sorry. From the photos, it looks like the front of the 3D printed phase plug is flat, and that there is a ring around the exit, perpendicular to the horn axis, where the printed part attaches to the wooden horn. If the taper of the wooden flare continues down at the same angle into the printed phase plug, so that there is no step, my comment was indeed wrong. |
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