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Downloads SPL and impedance response curves as text files
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TW022WA07/09 on-axis SPL response
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TW022WA07/09 impedance response
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TW022WA08/10 on-axis SPL response
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TW022WA08/10 impedance response
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Important! Please observe that these text files for download are actual measurements of the drivers measured in infinite baffle and without any enclosure. Measuring the drivers in a finite baffle (like the baffle of most speaker cabinets) and in any size of enclosure will lead to different response curves.
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NOMINAL SPECIFICATIONS
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Notes
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Parameter
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TW022WA07 TW022WA09
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TW022WA08 TW022WA10
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Unit
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Nominal size
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22
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22
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[mm]
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Nominal impedance
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4
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8
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[ohm]
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Recommended frequency range
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2 - 30
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2 - 30
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[kHz]
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1, 4
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Sensitivity, 2.83V/1m (average SPL in range 2 - 20 kHz)
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92
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89.5
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[dB]
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2
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Power handling, short term, IEC 268-5, 2.5 kHz@12dB/oct.
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700
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700
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[W]
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2
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Power handling, long term, IEC 268-5, 2.5 kHz@12dB/oct.
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70
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70
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[W]
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2
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Power handling, continuous, IEC 268-5, 2.5 kHz@12dB/oct.
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20
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20
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[W]
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Effective radiating area, Sd
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6.1
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6.1
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[sq.cm]
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3, 4, 6
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Resonance frequency (free air, no baffle), Fs
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700
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730
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[Hz]
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Moving mass, incl. air (free air, no baffle), Mms
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0.27
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0.25
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[g]
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3
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Force factor, Bxl
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1.76
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2.24
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[N/A]
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3, 4, 6
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Suspension compliance, Cms
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0.19
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0.19
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[mm/N]
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3, 4, 6
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Equivalent air volume, Vas
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10
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10
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[mlit.]
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3, 4, 6
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Mechanical resistance, Rms
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0.93
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0.93
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[Ns/m]
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3, 4, 6
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Mechanical Q, Qms
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1.3
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1.2
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[-]
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3, 4, 6
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Electrical Q, Qes
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1.2
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1.4
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[-]
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3, 4, 6
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Total Q, Qts
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0.62
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0.66
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[-]
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4
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Voice coil resistance, RDC
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3.1
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6.0
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[ohm]
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5
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Voice coil inductance, Le (measured at 20 kHz)
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22
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37
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[μH]
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Voice coil inside diameter
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22
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22
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[mm]
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Voice coil winding height
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1.8
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1.8
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[mm]
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Air gap height
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2.5
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2.5
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[mm]
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Theoretical linear motor stroke, Xmax
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+/-0.35
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+/-0.35
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[mm]
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Magnet weight
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18.5
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18.5
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[g]
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Total unit net weight excl. packaging
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77/94
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77/94
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[g]
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3, 4, 5
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Krm
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[mohm]
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3, 4, 5
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Erm
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[-]
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3, 4, 5
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Kxm
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[mH]
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3, 4, 5
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Exm
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[-]
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Note 1
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Measured in infinite baffle.
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Note 2
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Tested in free air (no cabinet).
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Note 3
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Measured using a semi-constant current source, nominal level 2 mA.
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Note 4
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Measured at 25 deg. C
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Note 5
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It is generally a rough simplification to assume that loudspeaker transducer voice coils exhibit the characteristics of an inductor. Instead it is a far more accurate approach to use the more advanced model often referred to as the “Wright empirical model”, also used in LEAP-4 as the TSL model (www.linearx.com), involving parameters Krm, Erm, Kxm, and Exm. This more accurate transducer model is described in a technical paper (PDF) here.
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Note 6
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Measured before burn in
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HARMONIC DISTORTION
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OUTLINE DRAWING AND NOMINAL DIMENSIONS
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PACKAGING AND ORDERING INFORMATION
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Part no. TW022WA07-01
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4 ohm version, without face plate, individual packaging (one pair per box)
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Part no. TW022WA07-02
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4 ohm version, without face plate, bulk (industrial) packaging
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Part no. TW022WA08-01
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8 ohm version, without face plate, individual packaging (one pair per box)
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Part no. TW022WA08-02
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8 ohm version, without face plate, bulk (industrial) packaging
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Part no. TW022WA09-01
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4 ohm version, with face plate, individual packaging (one pair per box)
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Part no. TW022WA09-02
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4 ohm version, with face plate, bulk (industrial) packaging
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Part no. TW022WA10-01
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8 ohm version, with face plate, individual packaging (one pair per box)
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Part no. TW022WA10-02
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8 ohm version, with face plate, bulk (industrial) packaging
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Latest update: October 10, 2020
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Specifications are subject to change without any further notice. Copyright © 2006-2022 by Wavecor Ltd., China. All rights reserved.
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MORE INFO
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