Mid-range beaming and narrowing

The Challenge of Midrange Response

In loudspeaker design, achieving a smooth and balanced frequency response across the entire spectrum is a continuous pursuit. One specific challenge lies in the midrange frequencies (typically around 1 kHz).

Here, two unwanted phenomena can significantly impact the sound and his power response: midrange narrowing and beaming.

Here we can see a not fully optimised end of profile resulting a narrowed mid-range in 1kHz region :

ideal CD

Whatever the horn, wageguide, integrated on baffle or not, the contour must be fluid in all directions.

Here is a very good elliptic waveguide with a slightly rounded traditional baffle where mid-range beaming and mid-range narrowing are still visible :
ideal CD
Then the same wave guide (but 0.5" tinier) integrated with a fluid profile :

ideal CD

Midrange Narrowing: A Dip Caused by Diffraction

Midrange narrowing refers to a decrease in sound pressure at specific midrange frequencies.

This occurs due to edge diffraction. When sound waves traveling from the driver encounter the sharp edges of the speaker baffle, they bend around these obstacles.

This bending disrupts the wavefront, causing destructive interference at certain wavelengths (frequencies). These wavelengths correspond to the dip observed in the midrange response of the speaker, affecting both on-axis and off-axis.

Here is an exemple about how to solve it:

next gen bi-radail

Midrange Beaming: Uneven Radiation Due to Diffraction

While midrange narrowing represents a loss of sound pressure, another effect of edge diffraction is midrange beaming. This phenomenon describes the concentration of sound pressure in specific off-axis directions.

The bending of sound waves can lead to constructive interference at certain angles, resulting in peaks in the off-axis response. However, in other off-axis locations, destructive interference can occur, causing dips.

This creates an uneven sound radiation pattern, compromising the overall soundstage and affecting listeners at various positions.

The Impact on Listening Experience

The combined effects of midrange narrowing and beaming can significantly alter the way we perceive sound. Here’s how:

Optimizing Baffle Design for Smooth Midrange

To address these challenges and achieve a smooth midrange response, loudspeaker designers employ various strategies:

4mm radius

For flat baffles, a simple round-over return might not be sufficient. In those cases, designers may employ profile acceleration and deceleration, this involves a gradual transition from the horn’s curvature to the flat surface of the baffle, minimizing the impact of abrupt changes on the wavefro

Advanced Design Techniques

Modern loudspeaker design tools like Finite Element Analysis (FEA) simulations allow for precise modeling of baffle shapes and their impact on sound radiation. This facilitates the optimization of baffle profiles to minimize diffraction effects and achieve a smooth, balanced midrange response.

Exception: Low midrange horns

Low midrange horns, typically wide horns (around 1 meter) used between 800 and 250 Hz, are a special case:

In this case, it’s more advantageous to exploit the midrange narrowing by introducing a more abrupt change. This will make the horn less usable above 900 Hz but will allow for a deeper horn, resulting in better loading.

This approach will also extend low-frequency control and loading as far as possible but is only applicable in this special case.

next gen bi-radail

Midrange Narrowing as a directivity control device

Free field:

A 15" driver’s directivity approximates horn directivity at crossover if the enclosure is just large enough to house the driver: The well placed 15" woofer box’s midrange narrowing, combined with the driver’s natural directivity, contributes to directivity control and proper wavefront propagation, it also allow the wavefront to leave the surface when needed so to not be torn.

If the baffle is too wide, the midrange narrowing shifts to an unwanted lower frequency.

For a mid-woofer, a well-placed midrange narrowing, in combination with the woofer’s natural directivity, allows the woofer’s directivity to match the horn’s directivity at the crossover.

This approach does not apply to compression driver horns or tweeters, where midrange narrowing must be minimized or eliminated.

In-Wall case:

In this case, the wall behaves as a 180° (or less in a corner) horn, providing very good constant directivity control at low frequencies. However, at the crossover frequency, it can cause a significant divergence between the directivity of the horn and the woofer. A flat wall will give around 140° when the horn should be close to 90°.

The temptation is huge to create a kind of corner at 90°, but the wavefront will not follow it, and we will simply add throat resonances on a large scale.

One of the solution can be this kind of device:

lens
The central part has no effect. The principle here is to take control on the horizontal part of the wavefront, guide it slightly, and simultaneously induce a midrange narrowing to achieve the desired directivity that matches high-frequency horn directivity.

It’s important to note that this device makes sense only in in-wall applications due to the wall directivity effect. In free-air, the solution described earlier in “Regular case” is at least as efficient and significantly simpler.

But there is a far simpler way.

In-Wall ideal case:

A simpler approach is to respect our Free field principles with a just large enought baffle and using an absorptive front wall following it. We avoid hard, hemispherical walls, as they create numerous early reflections directly upon sound propagation.

A wide, hard 2π wall (or baffle) distorts the wavefront because the baffle forces the sound energy to split, propagating both forward and in a 180° arc. Since the total energy remains constant, this splitting rapidly distorts then torn the wavefront at some point, paradoxically creating early reflections even on a flat surface.

In all cases, the front wall must be absorptive and flush with the speaker enclosure. It also plays a major role in room acoustics.

If the in-wall cannot be made of absorbing materials, use Free field solution as described will be preferable as the perception of the room or wall acting as a horn is an illusion.

Conclusion

Understanding midrange narrowing and beaming caused by edge diffraction is crucial for achieving optimal sound quality in loudspeakers. By employing careful baffle design techniques and advanced simulation tools, designers can create speakers that deliver a natural and detailed listening experience across the entire frequency spectrum, for both on-axis and off-axis listeners.

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