Formula: Axis of rotation
When something rotates, there will be a line where there is no movement. That is the axis of rotation. So when a player hits a forehand, the axis of rotation of the racquet will be between the middle and ring fingers, and perpendicular to the ground. Waggle a racquet in your hand and feel the alternating pressure on these two fingers, which predominate in the grip.
The shoulder is another axis of rotation, and this axis is used in computing Shoulder Pull.
On impact, there will be a resultant Torque about the hand axis of rotation, even if the impact is right on the sweet spot. Moment is a twist downward due to the racquet’s weight, and the axis of rotation for Moment is perpendicular to that for Torque, and parallel to the ground through the hand.
Yet another axis of rotation is along the centerline of the racquet (through the handle and the head), and it is about this axis that racquets will twist when the impact is off the centerline or even, due to the cross product of Moment and Torque, for impacts directly on the centerline. The twisting force about the centerline axis in the handle is known as Longitudinal Torque, or Torsion.
| \(A_x\) | = | Impulse Reaction, the translational force acting at the axis of rotation due to impact, in Newtons. Note that when \(d\) = \(q\) (\(q\) is the distance from the axis of rotation to the center of percussion), the expression within the second set of parentheses becomes zero. |
| \(a\) | = | linear acceleration of the mass center, in m/s² |
| \(b\) | = | mass of the ball, in kg |
| \(c\) | = | coefficient of restitution of the racquet/ball system |
| \(d\) | = | distance from the axis of rotation to the impact point, in cm |
| \(e\) | = | the distance from the axis of rotation to the tip |
| \(F\) | = | force applied at mass center, in Newtons |
| \(I\) | = | moment of inertia (swing weight) of racquet, in kgf/cm² |
| \(I_5\) | = | moment of inertia (swing weight) of racquet at 5cm from the butt, in kgf/cm² |
| \(I_7\) | = | moment of inertia (swing weight) of racquet at 7cm from the butt, in kgf/cm² |
| \(I_{10}\) | = | moment of inertia (swing weight) of racquet at 10cm from the butt, in kgf/cm² |
| \(I_a\) | = | moment of inertia (swing weight) of racquet at distance \(a\) from the butt, in kgf/cm² |
| \(M\) | = | mass of the racquet, in kg |
| \(m\) | = | mass in kg |
| \(ω\) | = | angular velocity of racquet, in radians/s |
| \(p\) | = | linear velocity of impact point, in m/s |
| \(r\) | = | distance in cm from mass center (balance point) to axis used in the stroke |
| \(s\) | = | ball velocity, in m/s (positive is away from player) |
| \(s_1\) | = | velocity of ball before impact, in m/s |
| \(s_2\) | = | velocity of ball after impact, in m/s |
| \(T\) | = | torque at axis of rotation, in Nms |
| \(t\) | = | dwell time, or duration of impact, in seconds |
| \(v\) | = | linear velocity of the mass center, in m/s |
| \(v_1\) | = | linear velocity, just before impact, of racquet mass center, in meters/second |
| \(v_2\) | = | linear velocity, just after impact, of racquet mass center, in meters/second |