Yuri G. PhD

Yuri G. PhD

Physics of Sports Research

Practical Application of Free Vibrations in a Single Tennis String

January 2008

Abstract

The purpose of this research is to establish the relationship between the frequency parameters of free vibrations of a tennis string, its length, and the applied tension force.

This analysis provides a theoretical foundation for optimizing string tensioning to achieve consistent performance across the entire string bed of a tennis racket.

Problem Formulation

To solve this problem, we consider a single string of length L₀, rigidly fixed at both ends with a pre-tensioned force T₀. To simplify the solution procedure, we examine the vibration of a string with a concentrated mass m, which is significantly greater than the mass of the string itself.

The solution is constructed for elastic vibrations of small amplitude.

Mathematical Model

The calculation scheme of the problem is presented in Figure 1. Two forces act on the string displaced from equilibrium:

T = T₀ + ΔT - Elastic deformation forces of the string

m·d²x/dt² - Inertial force of mass m movement

Where:

T₀ - Initial static tension of the string

ΔT - Elastic component of string tension caused by its displacement

String vibration model

Fig. 1 - String vibration model with concentrated mass

Mathematical Derivation

Equation of Motion

The equation of motion for the considered model, neglecting the mass of the string itself and resistance forces, has the form:

m·d²x/dt² + 2·(T₀ + ΔT)·sin(θ) = 0

Equation (1)

Small Oscillation Approximation

Considering small oscillations of the system, the deviation angle of mass m from the equilibrium position can be represented as:

sin(θ) ≈ θ = x / (L₀/2)

Introducing an intermediate function ξ = dx/dt, we transform the differential equation:

ξ·dξ/dx + (4T₀/(m·L₀))·x + (4ΔT/(m·L₀))·x = 0

Equation (2)

Integration and Boundary Conditions

Integrating appropriately and applying boundary conditions (zero velocity at maximum displacement), we obtain:

ξ² = (4T₀/(m·L₀))·(x_max² - x²) + (4ΔT/(m·L₀))·(x_max² - x²)

Equation (3)

Where x_max is the amplitude of oscillations.

Simplification for Small Angles

Considering the smallness of deviation angles, we simplify the equation to:

dξ/dx = - (2√(T₀/m)) / √(L₀·(x_max² - x²))

Equation (4)

Final Integration

Integrating equation (4), we find:

ξ = - (2√(T₀/m)) · arcsin(x/x_max) / √L₀ + C

Equation (5)

Substituting the expression for ξ = dx/dt, we obtain:

dx/dt = - (2√(T₀/m)) · arcsin(x/x_max) / √L₀ + C

Equation (6)

Frequency of Free Vibrations

Considering small oscillations, we can approximate:

arcsin(x/x_max) ≈ x/x_max

Then the frequency of free vibrations is determined by the expression:

Key Result: Natural Frequency Formula

f = (1/π) · √(T₀/(m·L₀))

Equation (7)

Practical Application

Analyzing formula (7), we can derive practical applications of the obtained solution. Specifically, to ensure equal compliance of strings of different lengths, it is sufficient to maintain equality of their free vibration frequencies.

This principle allows for:

  • Optimization of string tensioning patterns
  • Consistent ball response across the string bed
  • Improved control and predictability of shots
  • Better energy transfer from racket to ball

The relationship between tension, length, and vibration frequency provides a scientific basis for stringing techniques that enhance racket performance and player control.

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This analysis establishes the fundamental relationship between string tension, length, and vibration frequency

for optimized tennis racket performance.