Simulateur Torsion Balancer

Twistweight is perhaps the most critical metric for modern tennis, where players hit with heavy topspin and face high-velocity balls.

The Power of r²: The formula for the Moment of Inertia is I = mr², where m is mass and r is the distance from the center axis. Because the radius is squared, doubling the distance from the center doesn't just double the stability—it quadruples it.

The "Tightrope Walker" Effect: Imagine a tightrope walker holding a long pole. The pole isn't necessarily heavy, but because the weight is at the ends (extreme radius), it makes the walker incredibly hard to "tip" or twist.

In-Game Benefit: When a heavy ball hits the edge of your racket (3 or 9 o’clock), the racket wants to spin in your hand. Increasing TW provides the "torsional stiffness" required to keep the face of the racket pointing at your target instead of fluttering.

If Twistweight is about stability, Swingweight is about momentum. It determines how heavy the racket feels once it’s in motion.

Rotation from the Grip: Swingweight is calculated based on an axis 10cm up from the butt of the racket.

The 12 O’Clock Leverage: Mass added at the "tip" (12 o’clock) is at the maximum possible distance from your hand. This creates a massive "lever" effect. Even 2g at the tip can increase the Swingweight significantly, giving you more plow-through—the ability of the racket to "drive through" the ball without being pushed back.

The 3 & 9 O’Clock Sweet Spot: Placing mass at 3 and 9 o'clock is a "best of both worlds" approach. You are far enough from the center to increase Twistweight (stability), but close enough to the hand to keep the Swingweight increase manageable.

The percentage ranges and absolute values displayed represent the dynamic variability of your physical setup on the court.

Sweet Spot & Torsion (String Synergy): The upper bounds of our Sweet Spot and Twistweight metrics account for the strings you use. Thicker strings (like heavy polyesters) and lower tensions naturally amplify the metamaterial's dampening and stabilizing influence across the stringbed.

Swingweight (Placement & Aerodynamics): Unlike the other metrics, Swingweight increases are completely independent of your strings. Its range exists due to Placement Sensitivity—shifting the balancers just one cross-string up or down exponentially changes the result due to the squared distance (r²). Furthermore, placing a 3D-printed lattice at the fastest-moving part of the frame introduces slight aerodynamic drag, which increases the effective (dynamic) Swingweight during a full stroke beyond standard static math.