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W7
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W6v2
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W7 Technologies
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W7 Technologies: Ultra-Long Voice Coil
Summary:
To allow extreme linear excursion, phenomenal power handling and control, control, control.

Detailed Information:

The W7 voice coils are huge and by far the largest JL Audio has ever made (in diameter and winding height). The massive surface area of these coils is excellent for heat dissipation, while the huge winding height provides the necessary motivational force to achieve the huge excursion of the W7 designs.

Considering their size, the W7 voice coils are extremely light in weight. We use aluminum-alloy wire (instead of conventional copper) and a specific winding method to achieve the electrical properties that we deemed necessary to achieve our design goals. The light weight of the coils helps keep the overall moving mass down at manageable levels, which is extremely important for efficiency and sound quality reasons.

The 8W7 uses a 2.25-inch diameter coil (2.0-inch winding height), the 10W7 uses a 2.75-inch diameter coil (2.3-inch winding height), the 12W7 employs a 3-inch unit (2.8-inch winding height) and the 13W7 enters battle with a 3.55-inch diameter voice coil (3.0-inch winding height). You may have noticed that, for three of the W7's, we chose non-standard coil diameters. Because of the complete design freedom afforded us by the fact that we were willing and able to tool everything for these speakers, we were able to precisely specify the diameters that would produce optimum performance for each model.

Since the W7 is an extreme excursion speaker with a detachable surround, voice coil former resilience is a key parameter. If the surround is roughly handled, the coil former could be damaged by contact to the pole piece. Kapton� is a high temperature polyimide film that snaps back from moderate deformation without harm. Aluminum, however, will bend readily and stay that way. If an aluminum bobbin is deformed badly enough, it can lead to speaker failure (coil shorting or mechanically wedging in the magnetic gap.) Aluminum formers also create eddy-currents which lower the mechanical Q (Qms) and create additional heat, neither of which is a trait we were looking for in the W7 design. The modest power-handling advantage of an aluminum former pales in comparison to its practical incompatibility with the W7 design.
 
When a speaker is asked to handle the kind of power that a W7 is capable of handling, removing heat from the voice coil and motor parts becomes a big challenge, but one that has to be addressed in order to ensure reliability and sound quality. The vast majority of the power entering a woofer is converted directly to heat. The reason for this is that the speaker is a highly inefficient device. You may have heard that a typical amplifier is 50% efficient at rated power (this means that half of the power entering the amp is converted to heat). A typical, small-box woofer's efficiency (W7 included) runs at well under 1%, meaning that over 99% of the power you put into it becomes heat very quickly.
 







If the speaker is not capable of dissipating (getting rid of) heat in its voice coil, the voice coil will ultimately fail (burn). The amount of power that a speaker can handle continuously (we run them for eight hours) without burning its coil determines the thermal power handling of the design.
 
Even if you don't run a speaker hard enough to burn its coil, heat affects the speaker's performance in dramatic ways. As a voice coil heats up, its resistance rises, changing the speaker's impedance characteristics and making it even less efficient. This phenomenon is called power-compression and totally alters the speaker's high-power behavior if it isn't controlled. When power compression rears its ugly head, the speaker's dynamic range will be cut short and a loss of output will be experienced (compared to a cool speaker).
 
Because of the extreme power handling capability of the W7's, cooling was a major focus during the design phase. Our engineering team combined several technologies to effectively circulate air and remove heat from the voice coil and metal parts.
 
So why do the W7's use a 3 ohm voice coil?
 
We'll start by clarifying that the 8W7, 10W7 and 12W7 have single 3 ohm voice coils. The 13W7 has dual 1.5 ohm voice coils.

A single 3-ohm coil gave the best performance on the 8W7, 10W7 and 12W7 when balancing the critical parameters of voice coil mass, inductance, magnetic motor strength and coil impedance. Sound quality at extreme output levels was our ultimate goal and the voice coils needed to be precisely tailored to achieve it. The extreme nature of the W7 design does not leave as much flexibility to do multiple impedance versions as the lower series of JL Audio woofers. We realize that this will make it difficult to drive a single 8W7, 10W7 or 12W7 with some amplifiers optimized for low-impedance. Our decision was not some covert attempt to get consumers to buy JL Audio amplifiers (which can deliver full power at 3 ohms). It just worked out that 3 ohms was the best sounding solution for the 8W7, 10W7 and 12W7.

Any competent amplifier optimized for 4-ohms or 2-ohms mono will drive a single 8W7, 10W7 or 12W7 without any problem. With the 13W7 and its dual 1.5 ohm coils, there is greater amplifier application flexibility. The speaker may be configured as a 0.75-ohm woofer (coils in parallel), a 3 ohm woofer (coils in series), or it can be driven by two amplifiers, each driving one 1.5 ohm voice coil). In the future, as we continue developing the W7 platform, more impedance variations may be introduced.


 

 
     
 
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