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The anageometric Laplace transform has been formulated for scalar differential equations, but its use in coupled systems requires an explicit matrix-based treatment. This study applies the transform to linear systems of anageometric differential equations with constant coefficients and continuous forcing. The anageometric derivative is defined by D̃f(t) = t f′(t) for t ≥ 1, and the transform is taken with respect to the measure dt/t. Applying the derivative rule componentwise converts an initial value problem into a system of algebraic equations involving the matrix resolvent. A logarithmic change of time then yields an explicit solution formula and establishes uniqueness under the stated assumptions. Two coupled examples demonstrate the method. In a triangular system with forcing, inversion produces power-law terms together with a logarithmic term associated with a repeated transform-domain pole. In a two-component rotational system, the solutions are oscillatory functions of ln t and remain bounded. Direct substitution verifies the equations and initial conditions in both examples. The analysis shows precisely how classical linear-system tools transfer to the anageometric setting through logarithmic time. The matrix formulation also makes the effects of coupling visible in the transformed equations and in the resulting solutions. Its scope is limited to the system class and assumptions stated here; it does not claim a general solution method for nonlinear systems.
| Keywords | Anageometric Laplace transform; anageometric differential equations; coupled systems; matrix resolvent; logarithmic time. |
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| Mode | On-Site |