Mathematics / Muller's Method
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LABORATORY 06 · MATHEMATICS

Muller's Method lab report

A worked muller's method lab report with iteration data tables, logarithmic graphs, calculations, uncertainty and conclusions.

WORKED EXAMPLE · BENCHMARK OBSERVATIONS

A complete example laboratory report.

Simulated demonstration data.

This report illustrates formal numerical analysis, iteration tracking, and convergence rate extraction. Replace its observations with your own computational telemetry when preparing a practical submission.

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1. Title and aim

Parabolic Interpolation and Tribonacci Convergence of Muller's Method. Determine the roots of the cubic polynomial f(x) = x³ − x² − x − 1 = 0 using Muller's parabolic interpolation method, analyze 3-point quadratic curve fitting across consecutive iterates, and extract the theoretical Tribonacci superlinear convergence order α ≈ 1.839 via logarithmic linear regression.

2. Abstract

Six computational trials were executed across standardized inputs k = 1.0 to k = 6.0 for Parabolic Interpolation and Tribonacci Convergence of Muller's Method. An ordinary least-squares regression yielded an empirical Tribonacci Convergence Order α of 1.839 (difference from theoretical reference = 0.0001%). The empirical telemetry conclusively validates the theoretical model and complexity scaling with R² = 1.000000.

3. Apparatus and fixed settings

4. Theory and graph choice

Muller's method, devised in 1956 by American computer scientist David E. Muller, is a brilliant generalization of the secant method that bridges the gap between elementary root-finding and sophisticated polynomial algebra. While the secant method approximates a target function by a straight line passing through two points, Muller's method fits a second-degree polynomial—a parabola—through the three most recent approximations: (x_{k-2}, f(x_{k-2})), (x_{k-1}, f(x_{k-1})), and (x_k, f(x_k)). By modeling the local curvature of the function rather than merely its slope, Muller's method captures higher-order geometric features of the landscape. To find the next iterate, the algorithm solves for the intersection of this osculating parabola with the horizontal axis. To avoid the disastrous subtractive cancellation that plagues the standard textbook quadratic formula when b² >> 4ac, Muller formulated the root update using a rationalized alternative: x_{k+1} = x_k − 2c / [b ± √(b² − 4ac)], choosing the sign in the denominator to maximize its absolute magnitude. This elegant algebraic trick guarantees that the algorithm selects the parabolic root closest to the current iterate x_k. Furthermore, Muller's method possesses an extraordinary mathematical capability: when the interpolating parabola fails to cross the real horizontal axis, the discriminant b² − 4ac becomes negative, producing an imaginary square root. Consequently, Muller's method naturally generates complex numbers and can locate complex conjugate root pairs even when initialized with purely real starting guesses—a feat that neither bisection, Regula Falsi, nor the secant method can ever accomplish. The asymptotic error analysis of Muller's method leads to the celebrated Tribonacci characteristic equation: α³ − α² − α − 1 = 0, whose unique positive real root is the Tribonacci constant: α = (1/3)[1 + (19 + 3√33)^(1/3) + (19 − 3√33)^(1/3)] ≈ 1.839287. With an asymptotic convergence order of nearly 1.84, Muller's method converges far faster than the secant method (α ≈ 1.618) and approaches the lightning speed of Newton-Raphson while requiring only a single new function evaluation per step. In this computational laboratory, students investigate Muller's method applied to the Tribonacci cubic polynomial f(x) = x³ − x² − x − 1 = 0, linearize logarithmic error trajectories, and extract the theoretical Tribonacci convergence exponent α = 1.839, verifying the emergence of 3-point recurrence dynamics in numerical analysis.

\ln(\varepsilon_{k+1}) = \alpha \cdot \ln(\varepsilon_k) + \ln(C) \implies \alpha^3 - \alpha^2 - \alpha - 1 = 0 \implies \alpha \approx 1.839

The mathematical regression linearizes the relationship into the form y = mx + b. Here, the independent variable x represents Natural Log of Current Error ln(ε_k), and the dependent variable y represents Natural Log of Next Error ln(ε_{k+1}). The slope m directly extracts Tribonacci Convergence Order α, while the intercept b accounts for residual baseline offsets.

5. Method

  1. Select initial points x₀ = 2.500, x₁ = 2.000, and x₂ = 1.850. Evaluate f(x₀) = 5.875, f(x₁) = 1.000, and f(x₂) = 0.057375.
  2. Calculate step differences h₁ = x₁ − x₀ = −0.5, h₂ = x₂ − x₁ = −0.15. Compute divided differences δ₁ = (f(x₁) − f(x₀))/h₁ = 9.750, δ₂ = (f(x₂) − f(x₁))/h₂ = 6.28417.
  3. Calculate parabolic parameters: a = (δ₂ − δ₁)/(h₂ + h₁) = (−3.46583)/(−0.65) = 5.33205; b = a·h₂ + δ₂ = 5.33205·(−0.15) + 6.28417 = 5.48436; c = f(x₂) = 0.057375.
  4. Compute the discriminant: D = √(b² − 4ac) = √(30.0782 − 1.2237) = 5.37163. Select the denominator sign matching b: denom = b + sign(b)·D = 5.48436 + 5.37163 = 10.85599. Calculate next iterate: x₃ = x₂ − 2c / denom = 1.850 − 2(0.057375)/10.85599 = 1.839430.
  5. Compute error: ε₃ = |1.839430 − 1.839287| = 0.000143. Advance the 3-point window: {x₁, x₂, x₃} becomes the new triplet for the next step, yielding x₄ = 1.839286756 (ε₄ = 1.2 × 10⁻⁹).
  6. Perform linear regression of ln(ε_{k+1}) against ln(ε_k). Extract the empirical slope α = 1.83929, confirming the theoretical Tribonacci convergence order α ≈ 1.839.

6. Observations and calculation table

All iterative observations use strictly controlled 64-bit IEEE 754 precision buffers. Residuals are computed relative to the ordinary least-squares regression line.

Table 1. Six simulated observations; x and y represent transformed mathematical metrics.
No.Iteration Step k (steps)Muller Iterate x_k ()Natural Log of Current Error ln(ε_k)Natural Log of Next Error ln(ε_{k+1})Fitted yResidual
11.01.0-1.5000-2.9210-2.92100.0000
22.02.0-2.9210-5.5342-5.53420.0000
33.03.0-5.5342-10.3399-10.3399-0.0000
44.04.0-10.3399-19.1776-19.1776-0.0000
55.05.0-19.1776-35.4301-35.4301-0.0000
66.06.0-35.4302-65.3186-65.31860.0000

Download the sample observations (CSV) ↓

7. Worked calculation for one observation

For step k = 1.0: Current coordinate x = -1.5000. Mathematical model response y = -2.9210. Output reading: 1.0000.

8. Graph, gradient and final calculation

-74.68-39.50-54.40-28.98-34.12-18.47-13.84-7.956.442.57Natural Log of Current Error ln(ε_k)Natural Log of Next Error ln(ε_{k+1})

Circular markers represent empirical computational observations. The solid line represents the ordinary least-squares linear fit.

x̄ = -12.48382; ȳ = -23.12023
Σ(x − x̄)² = 836.32849
Σ(x − x̄)(y − ȳ) = 1538.00726
m = Σ(x − x̄)(y − ȳ) / Σ(x − x̄)² = 1.83899902
b = ȳ − mx̄ = -0.16250677
ln(ε_(k+1)) = 1.8390 · ln(ε_k) + -0.1625 ⟹ α = 1.839 (theoretical α = 1.839)

9. Uncertainty and comparison

Percentage difference = |estimate − theoretical value| / |theoretical value| × 100 = 0.0001%.

For n = 6 observations, Σresidual² = 1.4483e-09; s² = Σresidual²/(n − 2). Gradient standard error = √[s²/Σ(x − x̄)²] = 6.5797e-07. Intercept standard error = √[s²(1/n + x̄²/Σ(x − x̄)²)] = 1.1305e-05.

Propagating the fit parameters yields a fit standard error of 6.5797e-07 , with an ideal coefficient of determination R² = 1.000000.

In computational mathematics and numerical analysis, errors arise from algorithmic discretization, finite precision IEEE 754 floating-point arithmetic (machine epsilon ε_mach ≈ 2.22 × 10⁻¹⁶ for 64-bit double precision), and condition number propagation. The ordinary least-squares fit across n = 6 standardized observations provides standard errors for the gradient and intercept. Because the mathematical recurrence is evaluated with high numerical precision, the residual sum of squares is vanishingly small, yielding a coefficient of determination R² ≥ 0.999999 and confirming the theoretical mathematical model.

10. Result and discussion

Tribonacci Convergence Order α = 1.839
Theoretical reference value: 1.839

The empirical benchmark observations provide rigorous quantitative verification of Parabolic Interpolation and Tribonacci Convergence of Muller's Method. In numerical analysis, scientific computing, and computational mathematics, algorithms are characterized by their asymptotic operational scaling, stability, and convergence rates. Across all six observations, the empirical slope m = 1.8390 confirms the theoretical model with near-zero residual variance. Furthermore, comparison with alternative algorithmic paradigms underscores critical trade-offs between memory footprint, condition number sensitivity, and operational throughput. The algorithm's behavior confirms the mathematical predictions established by numerical analysis literature.

11. Precautions and limitations

Requires three initial approximations rather than one or two. The numerical simulation model evaluates the real root of f(x) = x³ − x² − x − 1 = 0 using Muller's method initialized at x₀ = 2.500, x₁ = 2.000, and x₂ = 1.850. Exact real root (the Tribonacci constant): x* = 1.839286755214161... Error trajectory across iterations: x₂ = 1.850000 (ε₂ = 0.010713), x₃ = 1.839430 (ε₃ = 1.433 × 10⁻⁴), x₄ = 1.839286756 (ε₄ = 1.250 × 10⁻⁹), x₅ = 1.839286755214 (ε₅ = 3.100 × 10⁻¹⁷). Logarithmic error coordinates: x = ln(ε_k) = [−1.5000, −4.5363, −8.8501, −20.4998] and y = ln(ε_{k+1}) = [−4.5363, −8.8501, −20.4998, −37.8631]. Ordinary least-squares linear regression on these coordinates produces an empirical slope α = 1.83929 and intercept ln(C) = −0.1625 with Pearson correlation coefficient R² = 0.999999997. The empirical convergence order α = 1.83929 matches the theoretical Tribonacci root α = 1.839287 with 0.0002% relative difference.

12. Conclusion

This computational laboratory investigation quantitatively verified the mathematical formulation and asymptotic scaling of Parabolic Interpolation and Tribonacci Convergence of Muller's Method. Through rigorous tracking across six observation points, we confirmed an empirical Tribonacci Convergence Order α of 1.839 matching the theoretical reference 1.839 within 0.0001% error. The investigation demonstrates why this method serves as an indispensable tool in modern computational science.