{"product_id":"m6-m3-m1-master-series-3-way-active-component-set","title":"M6.M3.M1 Master Series 3-way Active Component Set","description":"\u003ch1\u003eM6 Overview\u003c\/h1\u003e\n\u003cp\u003eThe Master Series M6 mid-woofer is a high stroke, low distortion high output mid-woofer.  This speaker features high stroke, low distortion, wide bandwidth, and high power handling.  It features a 51mm \/ 2” voice coil diameter for high power handling and motor force.\u003c\/p\u003e\n\u003cp\u003eThe M6 mid-woofer features a split-gap design which provides ±8.7mm of linear excursion, allowing for displacement equal to many 8 inch woofers. The high linear stroke features a flat BL curve for exceptional dynamics and impact.\u003c\/p\u003e\n\u003cp\u003eThe M6 has multiple copper shorting rings within its magnetic structure. These features result in exceptionally low inductance at all operational frequencies and across stroke.  This further extends bandwidth as well as reduces motional intermodulation distortion for a much more open and natural midrange.\u003c\/p\u003e\n\u003cp\u003eThe M6 uses a thermo-fused woven, strand-oriented-chain hardened polyolefin cone.  This cone features very high strength due to the strand orientation of the polyolefin monomer chains, and exceptional internal damping from the polyolefin itself.  The thermal fusing ensures an air-tight surface without degrading the woven feature and strand orientation.  The result is a cone with over 600 MPa of tensile strength, vastly superior internal damping as compared to carbon and glass fibers, and a density of just 0.9 g\/cm\u003csup\u003e3\u003c\/sup\u003e , approximately 40% that of carbon fiber.\u003c\/p\u003e\n\u003cp\u003eThe M6 basket is also extremely open and holds the motor structure at the rear, so that basket-based reflections back up to the cone are minimized.  Use of a shallow split gap motor structure and custom tooled basket, surround, cone, and spider result in a very shallow mounting depth so the mid-woofer can fit into shallow locations, enabling creative positioning for best acoustical performance.\u003c\/p\u003e\n\u003ch1\u003eM3 Overview\u003c\/h1\u003e\n\u003cp\u003eThe Master Series M3 midrange is a high stroke, low distortion wideband midrange.  This midrange has high stroke, very wide bandwidth, and high power handling.  It features a 38mm \/ 1.5” voice coil diameter for high power handling and motor force.\u003c\/p\u003e\n\u003cp\u003eThe M3midrange features a split-gap design which provides ±4.5mm of linear excursion, about double of most 75mm\/3 inch midranges. This lowers distortion over the operational range and allows a mid to play at least half an octave lower in frequency, allowing better imaging and sonic cohesion.\u003c\/p\u003e\n\u003cp\u003eThe M3 has multiple copper shorting rings within its magnetic structure. These features result in exceptionally low inductance at all operational frequencies and across stroke.  This further extends bandwidth as well as reduces motional inter-modulation distortion for a much more open and natural midrange.\u003c\/p\u003e\n\u003cp\u003eThe M3 uses a thermo-fused woven, strand-oriented-chain hardened polyolefin cone.  This cone features very high strength due to the strand orientation of the polyolefin monomer chains, and exceptional internal damping from the polyolefin itself.  The thermal fusing ensures an air-tight surface without degrading the woven feature and strand orientation.  The result is a cone with over 600 MPa of tensile strength, vastly superior internal damping as compared to carbon and glass fibers, and a density of just 0.9 g\/cm\u003csup\u003e3\u003c\/sup\u003e , approximately 40% that of carbon fiber.\u003c\/p\u003e\n\u003cp\u003eThe M3basket is also extremely open and holds the motor structure at the rear, so that basket-based reflections back up to the cone are minimized.  Use of a shallow split gap motor structure and custom tooled basket, surround, cone, and spider result in a very shallow mounting depth so the midrange can be placed as high as possible within a vehicle, to raise the stereo image up near the head of the listener.\u003c\/p\u003e\n\u003cp\u003eThe M3 comes with a chemically etched steel grille featuring an anti-resonant hole-pattern with size of opening optimized for dispersion.  The grille is mounted to the midrange with a friction-fit gasket ensuring vibration-free operation and eliminating visible screws.\u003c\/p\u003e\n\u003ch1\u003eM1 Overview\u003c\/h1\u003e\n\u003cp\u003eThe Master Series M1 tweeter is a high stroke, low distortion multilayer fabric dome 25mm tweeter.  This tweeter features exceptionally high stroke to allow lower crossover points without compression.\u003c\/p\u003e\n\u003cp\u003eThe M1 tweeter features a split-gap design which provides ±1.6mm of linear excursion, approximately 5 to 6 times that of most other tweeters. The result is a wider operational bandwidth – as low at 1500 Hz – and distortion reduced by up to a factor of 4.\u003c\/p\u003e\n\u003cp\u003eThe M1 use a specially developed dome material.  The dome’s fabric is a lamination of silk, polyester, and cotton and treated with a proprietary compound to unify the layers but allow each to provide their own unique benefits.  Silk adds the stretch\/pull basic mechanical strength; polyester provides rigidity of shape; cotton provides improved damping.\u003c\/p\u003e\n\u003cp\u003eThe M1 does not use a rear chamber to lower its resonance; instead, a larger roll surround provides a lower resonance of the driver.  This design allows for higher stroke as well, for full-range output down to 1500 Hz.  And by removing the rear chamber, resonances from that chamber are eliminated. The elimination of the rear chamber results in an 11.7mm (15\/32”) mounting depth for freedom of positioning.\u003c\/p\u003e\n\u003cp\u003eThe M1 comes with a chemically etched steel grille featuring an anti-resonant hole-pattern with size of opening optimized for dispersion.  The grille is mounted to the main tweeter with a friction-fit gasket ensuring vibration-free operation and eliminating visible screws.\u003c\/p\u003e\n\u003ch2\u003eM6 Crossover Frequency and power handling\u003c\/h2\u003e\n\u003cp\u003eThe M6 mid-woofer is a wide bandwidth, high stroke speaker.  A low pass crossover should be set no higher than 3500 Hz.  The actual value should be selected based upon the paired tweeter, midrange, or full-range speaker.\u003c\/p\u003e\n\u003cp\u003eThe bottom end is robust, and can often forego a subsonic filter.  The following table summarizes general guidelines about a subsonic filter.  As noted above, this is not a hard-and-fast set of limits, and the final installation needs to be considered when setting actual crossover values and gains.\u003c\/p\u003e\n\u003ctable\u003e\n\u003ctbody\u003e\n\u003ctr\u003e\n\u003ctd width=\"60\"\u003e\u003cstrong\u003ePower\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd width=\"138\"\u003e\u003cb\u003e6dB\/Oct\u003c\/b\u003e\u003c\/td\u003e\n\u003ctd width=\"144\"\u003e\u003cb\u003e12dB\/Oct\u003c\/b\u003e\u003c\/td\u003e\n\u003ctd width=\"165\"\u003e\u003cb\u003e18dB\/Oct\u003c\/b\u003e\u003c\/td\u003e\n\u003ctd width=\"117\"\u003e\u003cb\u003e24dB\/Oct\u003c\/b\u003e\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"60\"\u003e50W\u003c\/td\u003e\n\u003ctd width=\"138\"\u003eNot necessary\u003c\/td\u003e\n\u003ctd width=\"144\"\u003eNot necessary\u003c\/td\u003e\n\u003ctd width=\"165\"\u003eNot necessary\u003c\/td\u003e\n\u003ctd width=\"117\"\u003eNot necessary\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"60\"\u003e100W\u003c\/td\u003e\n\u003ctd width=\"138\"\u003eNot necessary\u003c\/td\u003e\n\u003ctd width=\"144\"\u003eNot necessary\u003c\/td\u003e\n\u003ctd width=\"165\"\u003eNot necessary\u003c\/td\u003e\n\u003ctd width=\"117\"\u003eNot necessary\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"60\"\u003e200W\u003c\/td\u003e\n\u003ctd width=\"138\"\u003e100 Hz\u003c\/td\u003e\n\u003ctd width=\"144\"\u003e80 Hz\u003c\/td\u003e\n\u003ctd width=\"165\"\u003e70 Hz\u003c\/td\u003e\n\u003ctd width=\"117\"\u003e60 Hz\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"60\"\u003e400W\u003c\/td\u003e\n\u003ctd width=\"138\"\u003e170 Hz\u003c\/td\u003e\n\u003ctd width=\"144\"\u003e135 Hz\u003c\/td\u003e\n\u003ctd width=\"165\"\u003e110 Hz\u003c\/td\u003e\n\u003ctd width=\"117\"\u003e100 Hz\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\n\u003c\/table\u003e\n\u003ch2\u003e\u003c\/h2\u003e\n\u003cp\u003eNote that with lower power applications, these frequencies may be adjusted down; with higher power, you may need to adjust the frequencies up.  Again, the actual implementation of the entire system needs to be considered when installing these products.  A small sealed chamber behind the midrange can increase mechanical power handling, but may negatively impact thermal power handling.\u003c\/p\u003e\n\u003ch2\u003eM3 Crossover Frequency and power handling\u003c\/h2\u003e\n\u003cp\u003eThe M3 midrange is a wideband, high stroke speaker.  A low pass filter for blending with a tweeter would be dependent upon the tweeter and location of tweeter and the M3.  As the M3 naturally rolls off above 12 kHz, it can often be used as a near-full-range speaker without a low pass filter applied.\u003c\/p\u003e\n\u003cp\u003eThe following table summarizes general guidelines for a high pass filter for use with the M3.  As noted above, this is not a hard-and-fast set of limits, and the final installation needs to be considered when setting actual crossover values and gains.\u003c\/p\u003e\n\u003ctable\u003e\n\u003ctbody\u003e\n\u003ctr\u003e\n\u003ctd width=\"60\"\u003e\u003cstrong\u003ePower\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd width=\"138\"\u003e\u003cb\u003e6dB\/Oct\u003c\/b\u003e\u003c\/td\u003e\n\u003ctd width=\"144\"\u003e\u003cstrong\u003e12dB\/Oct\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd width=\"165\"\u003e\u003cstrong\u003e18dB\/Oct\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd width=\"117\"\u003e\u003cb\u003e24dB\/Oct\u003c\/b\u003e\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"60\"\u003e50W\u003c\/td\u003e\n\u003ctd width=\"138\"\u003e250 Hz\u003c\/td\u003e\n\u003ctd width=\"144\"\u003e225 Hz\u003c\/td\u003e\n\u003ctd width=\"165\"\u003e200 Hz\u003c\/td\u003e\n\u003ctd width=\"117\"\u003e160 Hz\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"60\"\u003e100W\u003c\/td\u003e\n\u003ctd width=\"138\"\u003e400 Hz\u003c\/td\u003e\n\u003ctd width=\"144\"\u003e300 Hz\u003c\/td\u003e\n\u003ctd width=\"165\"\u003e250 Hz\u003c\/td\u003e\n\u003ctd width=\"117\"\u003e225 Hz\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"60\"\u003e200W\u003c\/td\u003e\n\u003ctd width=\"138\"\u003e450 Hz\u003c\/td\u003e\n\u003ctd width=\"144\"\u003e350 Hz\u003c\/td\u003e\n\u003ctd width=\"165\"\u003e325 Hz\u003c\/td\u003e\n\u003ctd width=\"117\"\u003e300 Hz\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"60\"\u003e400W\u003c\/td\u003e\n\u003ctd width=\"138\"\u003eNot Recommended\u003c\/td\u003e\n\u003ctd width=\"144\"\u003eNot Recommended\u003c\/td\u003e\n\u003ctd width=\"165\"\u003e400 Hz\u003c\/td\u003e\n\u003ctd width=\"117\"\u003e350 Hz\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\n\u003c\/table\u003e\n\u003ch2\u003e\u003c\/h2\u003e\n\u003cp\u003eNote that with lower power applications, these frequencies may be adjusted down; with higher power, you may need to adjust the frequencies up.  Again, the actual implementation of the entire system needs to be considered when installing these products.  A small sealed chamber behind the midrange can increase mechanical power handling, but may negatively impact thermal power handling.\u003c\/p\u003e\n\u003ch2\u003eM1 Crossover Frequency and power handling\u003c\/h2\u003e\n\u003cp\u003eThe M1 Tweeter is a wideband, high stroke tweeter.  This gives it quite a bit of flexibility in operation.  The following table summarizes general guidelines.  As noted above, this is not a hard-and-fast set of limits, and the final installation needs to be considered when setting actual crossover values and gains.\u003c\/p\u003e\n\u003ctable\u003e\n\u003ctbody\u003e\n\u003ctr\u003e\n\u003ctd width=\"60\"\u003e\u003cstrong\u003ePower\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd width=\"138\"\u003e\u003cstrong\u003e6dB\/Oct\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd width=\"144\"\u003e\u003cstrong\u003e12dB\/Oct\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd width=\"165\"\u003e\u003cstrong\u003e18dB\/Oct\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd width=\"117\"\u003e\u003cstrong\u003e24dB\/Oct\u003c\/strong\u003e\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"60\"\u003e50W\u003c\/td\u003e\n\u003ctd width=\"138\"\u003e2000 Hz\u003c\/td\u003e\n\u003ctd width=\"144\"\u003e1750 Hz\u003c\/td\u003e\n\u003ctd width=\"165\"\u003e1500 Hz\u003c\/td\u003e\n\u003ctd width=\"117\"\u003e1200 Hz\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"60\"\u003e100W\u003c\/td\u003e\n\u003ctd width=\"138\"\u003e2800 Hz\u003c\/td\u003e\n\u003ctd width=\"144\"\u003e2200 Hz\u003c\/td\u003e\n\u003ctd width=\"165\"\u003e2000 Hz\u003c\/td\u003e\n\u003ctd width=\"117\"\u003e1800 Hz\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"60\"\u003e200W\u003c\/td\u003e\n\u003ctd width=\"138\"\u003e4500 Hz\u003c\/td\u003e\n\u003ctd width=\"144\"\u003e3500 Hz\u003c\/td\u003e\n\u003ctd width=\"165\"\u003e2600 Hz\u003c\/td\u003e\n\u003ctd width=\"117\"\u003e2350 Hz\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"60\"\u003e400W\u003c\/td\u003e\n\u003ctd width=\"138\"\u003eNot Recommended\u003c\/td\u003e\n\u003ctd width=\"144\"\u003eNot Recommended\u003c\/td\u003e\n\u003ctd width=\"165\"\u003eNot Recommended\u003c\/td\u003e\n\u003ctd width=\"117\"\u003e4000 Hz\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\n\u003c\/table\u003e\n\u003cp\u003eNot that with lower power applications, these frequencies may be adjusted down; with higher power, you may need to adjust the frequencies up.  Again, the actual implementation of the entire system needs to be considered when installing these products.\u003c\/p\u003e\n\u003ch2\u003eM6 Response\u003c\/h2\u003e\n\u003cp\u003e\u003cimg class=\"alignnone size-large wp-image-5202\" src=\"https:\/\/adcaraudio.com\/store\/wp-content\/uploads\/M6-frequency-respose-from-Klippel-1024x497.jpg\" alt=\"\" width=\"900\" height=\"437\"\u003e\u003c\/p\u003e\n\u003ch2\u003eM3 Response\u003c\/h2\u003e\n\u003cp\u003e \u003c\/p\u003e\n\u003ch2\u003e\u003cimg class=\"alignnone size-large wp-image-5205\" src=\"https:\/\/adcaraudio.com\/store\/wp-content\/uploads\/M3-frequency-graph-1024x492.jpg\" alt=\"\" width=\"900\" height=\"432\"\u003e\u003c\/h2\u003e\n\u003ch2\u003eM1 Response\u003c\/h2\u003e\n\u003ch2\u003e\u003cimg class=\"alignnone size-large wp-image-5208\" src=\"https:\/\/adcaraudio.com\/store\/wp-content\/uploads\/M1-frequency-response-1024x497.jpg\" alt=\"\" width=\"900\" height=\"437\"\u003e\u003c\/h2\u003e\n\u003cp\u003e\u003cimg class=\"alignnone size-large wp-image-5201\" src=\"https:\/\/adcaraudio.com\/store\/wp-content\/uploads\/M6-dimensions-945x1024.jpg\" alt=\"\" width=\"900\" height=\"975\"\u003e\u003c\/p\u003e\n\u003cp\u003e\u003cimg class=\"alignnone size-large wp-image-5204\" src=\"https:\/\/adcaraudio.com\/store\/wp-content\/uploads\/M3-dimensions-779x1024.jpg\" alt=\"\" width=\"779\" height=\"1024\"\u003e\u003c\/p\u003e\n\u003cp\u003e\u003cimg class=\"alignnone size-large wp-image-5207\" src=\"https:\/\/adcaraudio.com\/store\/wp-content\/uploads\/M1-dimensions-966x1024.jpg\" alt=\"\" width=\"900\" height=\"954\"\u003e\u003c\/p\u003e\n\u003ch2\u003eM6 Thiele Small Parameters\u003c\/h2\u003e\n\u003ctable\u003e\n\u003ctbody\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eNominal Impedance\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e4 Ohms\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eNominal SPL\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e86 dB @ 1W, 1m (89 dB @ 2.83Vrms, 1m)\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eResonant Frequency (Fs)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e65 Hz ±10%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eTotal System Q (Qts)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e0.75±15%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eEquivalent Volume Air (Vas)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e8 liters  ±15%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eMotor Force (BL)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e5.8 N\/A  ±10%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eInductance (Le)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e0.110mH±5%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eDC Resistance (DCR)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e3.8 Ohms  ±5%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eMoving Mass (Mms)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e21 grams  ±10%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eElectrical Q (Qes)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e0.95±10%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eMechanical Q (Qms)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e3.5±15%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eDiaphragm Surface Area (Sd)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e133 cm²±2%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eLinear Excursion (Xmax)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e8.7mm one way  ±5%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\n\u003c\/table\u003e\n\u003ch2\u003e\u003c\/h2\u003e\n\u003ch2\u003eM3 Thiele Small Parameters\u003c\/h2\u003e\n\u003ctable\u003e\n\u003ctbody\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eNominal Impedance\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e4 Ohms\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eNominal SPL\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e84 dB @ 1W, 1m (87 dB @ 2.83Vrms, 1m)\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eResonant Frequency (Fs)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e149 Hz ±10%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eTotal System Q (Qts)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e1.3±15%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eEquivalent Volume Air (Vas)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e0.5 liters  ±15%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eMotor Force (BL)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e2.7 N\/A  ±10%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eInductance at 1 kHz (Le)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e0.08 mH  ±5%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eDC Resistance (DCR)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e3.3 Ohms  ±5%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eMoving Mass (Mms)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e4.7 grams  ±10%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eElectrical Q (Qes)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e1.6±10%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eMechanical Q (Qms)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e6.3±15%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eDiaphragm Surface Area (Sd)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e39 cm²±2%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eLinear Excursion (Xmax)\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e4.5mm one way  ±5%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\n\u003c\/table\u003e\n\u003ch2\u003e\u003c\/h2\u003e\n\u003ch2\u003eM1 Thiele Small Parameters\u003c\/h2\u003e\n\u003ctable\u003e\n\u003ctbody\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eImpedance\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e4 Ohms\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eNominal SPL\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e89 dB @ 1W, 1m (92 dB @ 2.83Vrms, 1m)\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eResonant Frequency\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e1500 Hz ±10%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eTHD @ 100 dB, 4\u003csup\u003eth\u003c\/sup\u003e order high pass @ 1500 Hz\u003c\/td\u003e\n\u003ctd width=\"312\"\u003eLess than 1%, 1 meter\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd width=\"312\"\u003eMax power handling\u003c\/td\u003e\n\u003ctd width=\"312\"\u003e400W, 4\u003csup\u003eth\u003c\/sup\u003e order high pass @ 4000 Hz\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\n\u003c\/table\u003e\n\u003ch2\u003e\u003c\/h2\u003e","brand":"Audio Dynamics","offers":[{"title":"Default Title","offer_id":52549562237159,"sku":"M6.M3.M1","price":2089.0,"currency_code":"USD","in_stock":true}],"url":"https:\/\/www.mediocrecustoms.com\/products\/m6-m3-m1-master-series-3-way-active-component-set","provider":"Mediocre Customs","version":"1.0","type":"link"}