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WOOFER 12WS600 - jbl selenium

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RESPONSE CURVES (0° AND 45°) IN A TEST ENCLOSURE INSIDE AN<br />

ANECHOIC CHAMBER, 1 W / 1 m<br />

110<br />

100<br />

POLAR RESPONSE CURVES<br />

60°<br />

30°<br />

50 Hz<br />

0<br />

-6<br />

-10<br />

330°<br />

300°<br />

<strong>WOOFER</strong><br />

<strong>12WS600</strong><br />

60°<br />

30°<br />

100 Hz<br />

0<br />

-6<br />

-10<br />

250 Hz<br />

-20<br />

-20<br />

-20<br />

90° dB<br />

270° 90° dB<br />

270° 90° dB<br />

270°<br />

330°<br />

300°<br />

60°<br />

30°<br />

0<br />

-6<br />

-10<br />

330°<br />

300°<br />

90<br />

120°<br />

240°<br />

120°<br />

240°<br />

120°<br />

240°<br />

dB<br />

80<br />

150°<br />

180°<br />

210°<br />

150°<br />

180°<br />

210°<br />

150°<br />

180°<br />

210°<br />

70<br />

30°<br />

500 Hz<br />

0<br />

-6<br />

330°<br />

30°<br />

800 Hz<br />

0<br />

-6<br />

330°<br />

30°<br />

1.25 kHz<br />

0<br />

-6<br />

330°<br />

60°<br />

-10<br />

300°<br />

60°<br />

-10<br />

300°<br />

60°<br />

-10<br />

300°<br />

60<br />

20 200<br />

Hz<br />

2k 20k<br />

Response Curve at 0°.<br />

Response Curve at 45°.<br />

-20<br />

90° dB<br />

270°<br />

120°<br />

150°<br />

180°<br />

210°<br />

240°<br />

-20<br />

90° dB<br />

270°<br />

120°<br />

150°<br />

180°<br />

210°<br />

240°<br />

-20<br />

90° dB<br />

270°<br />

120°<br />

150°<br />

180°<br />

210°<br />

240°<br />

IMPEDANCE AND PHASE CURVES MEASURED IN FREE-AIR<br />

400<br />

90<br />

30°<br />

2 kHz 3.15 kHz<br />

0<br />

-6<br />

330°<br />

30°<br />

0<br />

-6<br />

330°<br />

60°<br />

-10<br />

300°<br />

60°<br />

-10<br />

300°<br />

300<br />

45<br />

-20<br />

90° dB<br />

270°<br />

-20<br />

90° dB<br />

270°<br />

ohms<br />

200<br />

0<br />

degrees<br />

120°<br />

150°<br />

180°<br />

210°<br />

240°<br />

120°<br />

150°<br />

180°<br />

210°<br />

240°<br />

Polar Response Curve.<br />

100<br />

-45<br />

HARMONIC DISTORTION CURVES MEASURED AT 10% AES INPUT<br />

POWER, 1 m<br />

dB<br />

140<br />

120<br />

100<br />

0<br />

-90<br />

20 200 2k 20k<br />

Hz<br />

Impedance Curve.<br />

Phase Curve.<br />

80<br />

HOW TO CHOOSE THE RIGHT AMPLIFIER<br />

The power amplifier must be able to supply twice the RMS driver power. This<br />

3 dB headroom is necessary to handle the peaks that are common to<br />

musical programs. When the amplifier clips those peaks, high distortion<br />

arises and this may damage the transducer due to excessive heat. The use<br />

of compressors is a good practice to reduce music dynamics to safe levels.<br />

FINDING VOICE COIL TEMPERATURE<br />

It is very important to avoid maximum voice coil temperature. Since moving<br />

coil resistance (R E) varies with temperature according to a well known law,<br />

we can calculate the temperature inside the voice coil by measuring the<br />

voice coil DC resistance:<br />

T<br />

B<br />

T<br />

A<br />

R<br />

<br />

<br />

R<br />

B<br />

A<br />

<br />

1<br />

<br />

T<br />

<br />

1 <br />

25 <br />

<br />

25<br />

<br />

T A , T B= voice coil temperatures in °C.<br />

R A , R B= voice coil resistances at temperatures T A and T B, respectively.<br />

= voice coil wire temperature coefficient at 25 °C.<br />

POWER COMPRESSION<br />

Voice coil resistance rises with temperature, which leads to efficiency<br />

reduction. Therefore, if after doubling the applied electric power to the driver<br />

we get a 2 dB rise in SPL instead of the expected 3 dB, we can say that<br />

power compression equals 1 dB. An efficient cooling system to dissipate<br />

voice coil heat is very important to reduce power compression.<br />

A<br />

60<br />

20<br />

200 2k<br />

20k<br />

Hz<br />

Response Curve.<br />

Distortion Curve, 2nd harmonic.<br />

Distortion Curve, 3rd harmonic.<br />

NON-LINEAR VOICE COIL PARAMETERS<br />

Due to its close coupling with the magnetic assembly, the voice coil in<br />

electrodynamic loudspeakers is a very non-linear circuit. Using the nonlinear<br />

modeling parameters Krm, Kxm, Erm and Exm from an empirical<br />

model, we can calculate voice coil impedance with good accuracy.<br />

SUGGESTED PROJECTS<br />

VB1205B1 VB1205D1 HB1205A1 HB1205A3 HB1205D1<br />

For additional project suggestions, please access our website.<br />

TEST ENCLOSURE<br />

35-liter volume with a duct ø 3” by 1.97” length.<br />

Devido aos avanços tecnológicos, reservamo-nos<br />

o direito de inserir modificações sem prévio aviso.<br />

Cód.: 28026133 Rev.: 00 - 01 / 06<br />

www.<strong>selenium</strong>.com.br<br />

www.<strong>selenium</strong>loudspeakers.com

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