Wavecor TW030WA11

30 mm, wave guide, chamber, optim. textile dome, ferrite, 4 ohm
Beschikbaarheid:: Niet op voorraad
Artikelnummer voorraad referentie: 1381248
Leveringsdatum: Direct leverbaar
Fabrikant: Wavecor
€62,91 incl. BTW
Exclusief verzenden

TW030WA11 and TW030WA12 are tweeters designed for the most demanding applications, where low resonance frequency, high sensitivity and power handling, controlled dispersion, and a very wide frequency range are required.

Features

  • Featuring waveguide face plate for controlled dispersion, offering optimized off-axis and power response
  • 30 mm voice coil design with high power handling, and low resonance frequency
  • Copper clad center pole yielding very low voice coil inductance for reduced distortion and increased high frequency output
  • Internal volumes for low resonance frequency and distortion
  • Precision-coated textile diaphragm for improved consistency and high-frequency extension
  • Optimized dome shape for ultra high frequency cutoff
  • Vented voice coil former for reduced distortion and compression
  • Copper-clad aluminium voice coil wire offering lower moving mass for improved efficiency and transient response
  • Build-in cavities under dome/edge to equalize pressure for lower distortion and lower resonance frequency
  • Flexible lead wires for higher power handling and larger excursion
  • Gold plated terminals to prevent oxidation and ensure long-term reliable connection
  • Delivered with foam gasket attached for hassle-free mounting and secure cabinet sealing

Nominal specifications

Notes

  Parameter

TW030WA11

TW030WA12

Unit

Nominal size

30

30

[mm]

Nominal impedance

4

8

[ohm]

Recommended frequency range

1.5 - 25

1.5 - 25

[kHz]

1, 4

Sensitivity, 2.83V/1m (average SPL in range 2 - 20 kHz)

93.5

91

[dB]

2

Power handling, short term, IEC 268-5, 2.5 kHz@12dB/oct.

[W]

2

Power handling, long term, IEC 268-5, 2.5 kHz@12dB/oct.

[W]

2

Power handling, continuous, IEC 268-5, 2.5 kHz@12dB/oct.

45

45

[W]

Effective radiating area, Sd

11.5

11.5

[sq.cm]

3, 4, 6

Resonance frequency (free air, no baffle), Fs

410

425

[Hz]

Moving mass, incl. air (free air, no baffle), Mms

0.43

0.40

[g]

3

Force factor, Bxl

1.7

2.0

[N/A]

3, 4, 6

Suspension compliance, Cms

0.35

0.35

[mm/N]

3, 4, 6

Equivalent air volume, Vas

66

66

[mlit.]

3, 4, 6

Mechanical resistance, Rms

0.57

0.57

[Ns/m]

3, 4, 6

Mechanical Q, Qms

1.9

1.9

[-]

3, 4, 6

Electrical Q, Qes

1.34

1.74

[-]

3, 4, 6

Total Q, Qts

0.79

0.90

[-]

4

Voice coil resistance, RDC

3.5

6.5

[ohm]

5

Voice coil inductance, Le (measured at 20 kHz)

23

35

[μH]

Voice coil inside diameter

30.4

30.4

[mm]

Voice coil winding height

1.7

1.7

[mm]

Air gap height

2.5

2.5

[mm]

Theoretical linear motor stroke, Xmax

±0.40

±0.40

[mm]

Magnet weight

[g]

Total unit net weight excl. packaging

0.70

0.70

[kg]

3, 4, 5

Krm

2.9

2.8

[mohm]

3, 4, 5

Erm

0.50

0.53

[-]

3, 4, 5

Kxm

58

424

[mH]

3, 4, 5

Exm

0.20

0.036

[-]

Note 1.  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.

Specifications are before burn-in

Product Informatie PDF

Download PDF data sheet

TW030WA11 and TW030WA12 are tweeters designed for the most demanding applications, where low resonance frequency, high sensitivity and power handling, controlled dispersion, and a very wide frequency range are required.

Features

  • Featuring waveguide face plate for controlled dispersion, offering optimized off-axis and power response
  • 30 mm voice coil design with high power handling, and low resonance frequency
  • Copper clad center pole yielding very low voice coil inductance for reduced distortion and increased high frequency output
  • Internal volumes for low resonance frequency and distortion
  • Precision-coated textile diaphragm for improved consistency and high-frequency extension
  • Optimized dome shape for ultra high frequency cutoff
  • Vented voice coil former for reduced distortion and compression
  • Copper-clad aluminium voice coil wire offering lower moving mass for improved efficiency and transient response
  • Build-in cavities under dome/edge to equalize pressure for lower distortion and lower resonance frequency
  • Flexible lead wires for higher power handling and larger excursion
  • Gold plated terminals to prevent oxidation and ensure long-term reliable connection
  • Delivered with foam gasket attached for hassle-free mounting and secure cabinet sealing

Nominal specifications

Notes

  Parameter

TW030WA11

TW030WA12

Unit

Nominal size

30

30

[mm]

Nominal impedance

4

8

[ohm]

Recommended frequency range

1.5 - 25

1.5 - 25

[kHz]

1, 4

Sensitivity, 2.83V/1m (average SPL in range 2 - 20 kHz)

93.5

91

[dB]

2

Power handling, short term, IEC 268-5, 2.5 kHz@12dB/oct.

[W]

2

Power handling, long term, IEC 268-5, 2.5 kHz@12dB/oct.

[W]

2

Power handling, continuous, IEC 268-5, 2.5 kHz@12dB/oct.

45

45

[W]

Effective radiating area, Sd

11.5

11.5

[sq.cm]

3, 4, 6

Resonance frequency (free air, no baffle), Fs

410

425

[Hz]

Moving mass, incl. air (free air, no baffle), Mms

0.43

0.40

[g]

3

Force factor, Bxl

1.7

2.0

[N/A]

3, 4, 6

Suspension compliance, Cms

0.35

0.35

[mm/N]

3, 4, 6

Equivalent air volume, Vas

66

66

[mlit.]

3, 4, 6

Mechanical resistance, Rms

0.57

0.57

[Ns/m]

3, 4, 6

Mechanical Q, Qms

1.9

1.9

[-]

3, 4, 6

Electrical Q, Qes

1.34

1.74

[-]

3, 4, 6

Total Q, Qts

0.79

0.90

[-]

4

Voice coil resistance, RDC

3.5

6.5

[ohm]

5

Voice coil inductance, Le (measured at 20 kHz)

23

35

[μH]

Voice coil inside diameter

30.4

30.4

[mm]

Voice coil winding height

1.7

1.7

[mm]

Air gap height

2.5

2.5

[mm]

Theoretical linear motor stroke, Xmax

±0.40

±0.40

[mm]

Magnet weight

[g]

Total unit net weight excl. packaging

0.70

0.70

[kg]

3, 4, 5

Krm

2.9

2.8

[mohm]

3, 4, 5

Erm

0.50

0.53

[-]

3, 4, 5

Kxm

58

424

[mH]

3, 4, 5

Exm

0.20

0.036

[-]

Note 1.  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.

Specifications are before burn-in

Product Informatie PDF

Download PDF data sheet

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