Speakers. The last opportunity to modify your tone. Unlike hi-fi speakers which attempt to create sounds that are true to the musical source fed them, guitar speakers impart their own tone.
Your amp/cabinet pretty much determines three things about what speaker to select; speaker size, impedance and power rating. (See our tech corner article on Speaker Impedance, Power Handling and Wiring). But the tone is up to you! Speaker replacement is probably the easiest mod you can perform.
Sound Reinforcement - 18 inch Subwoofer. The Low Rider driver series represents a milestone in highpowered sub-woofer design. An incredible 1,600 Watt program rating and extra-long cone excursion provide maximum amounts of amazingly clean, deep bass.
The 1801 is an 8 ohm, 18" Black Widow/Super Structure speaker which offers the ultimate in deep, extended, bass response while maintaining a high sensitivity and high power capability. This is the woofer of choice for discos subwoofers, special effects, or anywhere low end punch and impact are a must! A long throw voice coil and Kevlar impregnated cone team up for excellent linearity.
Peavey Black Widow Super Structure Replacement Basket (1801-8 LT BW™ RB, 8 Ohm). Replaceable baskets eliminate the need for re-coning speakers and the frustration and delays associated with the re-coning process. It only takes a few minutes to replace a basket and you are back in business.
18" ferrite magnet, cast aluminium chassis LF driver delivering 700Wrms (AES Standard) power handling and 94dB sensitivity
3" high temperature, multi-layer voice coil for greater motor force
FEA optimized magnet assembly and suspension deliver highly symmetrical cone movement, leading to exceptionally low harmonic distortion
Balanced Airflow Venting (BAV) on the front-plate increases airflow to provide enhanced cooling
Dual Magnet Motor (DMM) incorporates a secondary magnet used to increase overall motor force (Bl) without the need for any additional increase in magnet size
“Multi-roll” surround provides exceptional linearity at extremes of cone excursion
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