Trailer: https://www.youtube.com/watch?v=bbkxoHI_QSM
Blog: http://www.rocketleague.com/news/the-bugatti-centodieci-redefines-power/
ELEGANT, SCULPTURAL, AND JAW-DROPPINGLY QUICK
Humans love speed. From childhood cheetah facts to the ever-popular “race you there!” challenge, we have an innate infatuation with going fast. French hypercar manufacturer Bugatti has always understood this. With record-breaking hypercars like the Veyron and Chiron, Bugatti has captured the hearts of gearheads for decades. Now, they’re bringing that same heat to Rocket League!
Obtain beautiful speed with the 90s-inspired Bugatti Centodieci Bundle, available for 1100 Credits from December 19 to January 3.
BUGATTI CENTODIECI
With a power output of 1177 kW/1600 horsepower, the Bugatti Centodieci represents peak hypercar performance, but it also takes a great deal of design inspiration from its namesake: the EB110.
Sporting a modern version of the iconic horseshoe grille, the original EB110 defined a new generation of Bugatti. When it first launched in 1991, the EB110 was the fastest production car in the world. Today’s Centodieci is just as extraordinary, with an ultra-limited run of only ten vehicles made. Luckily, the Rocket League version has the same sculptural look and is much easier to get!
The Hitbox with the lowest profile makes a long-awaited return! That’s right, the Centodieci’s aerodynamic stance makes the car a perfect fit for the in-game Plank Hitbox. Equip the matching Decal, Player Banner, and Engine Audio for the ultimate Bugatti experience.
BUGATTI CENTODIECI BUNDLE (1100 CREDITS)
- Bugatti Centodieci Body (Plank hitbox)
- Noire Decal
- Bugatti Centodieci Wheels
- Bugatti Centodieci Engine Audio
- Bugatti Centodieci Player Banner
\Note: Items included in the bundle can only be equipped by the Bugatti Centodieci. The Bugatti Centodieci cannot be customized with other branded content. Car colors cannot be adjusted while using the Noire Decal.*
Ready to go fast? Pick up the Bugatti Centodieci Bundle from December 19 to January 3.
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