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Ordinary Differential Equations
Table of Contents

Systems of linear differential equations can include external forces or inputs. These nonhomogeneous systems require special techniques to solve, combining solutions from the homogeneous system with particular solutions that account for the external influences.

Solving nonhomogeneous systems is crucial for understanding real-world applications like forced oscillations and resonance. These phenomena occur when external forces act on oscillating systems, potentially leading to amplified responses or even system failure if not properly managed.

Nonhomogeneous Systems and Solutions

Characteristics of Nonhomogeneous Systems

  • Nonhomogeneous systems contain an inhomogeneous term, which is a function that depends on the independent variable (usually time $t$)
  • The inhomogeneous term represents an external force or input acting on the system
  • The presence of the inhomogeneous term makes the system nonhomogeneous and changes the nature of its solutions
  • The general solution to a nonhomogeneous system consists of the sum of the complementary solution (solution to the corresponding homogeneous system) and a particular solution

Particular Solutions

  • A particular solution is a specific solution to the nonhomogeneous system that satisfies the differential equation
  • The particular solution accounts for the effect of the inhomogeneous term on the system's behavior
  • The particular solution is not unique; there are infinitely many particular solutions for a given nonhomogeneous system
  • The choice of a particular solution depends on the method used to solve the system and the form of the inhomogeneous term
  • The particular solution, when added to the complementary solution, provides the general solution to the nonhomogeneous system

Methods for Solving Nonhomogeneous Systems

Method of Undetermined Coefficients

  • The method of undetermined coefficients is used when the inhomogeneous term is a polynomial, exponential, sine, cosine, or a combination of these functions
  • Assume a particular solution with unknown coefficients that has the same form as the inhomogeneous term
    • For a polynomial inhomogeneous term, assume a polynomial particular solution
    • For an exponential inhomogeneous term, assume an exponential particular solution
    • For a sinusoidal inhomogeneous term, assume a sinusoidal particular solution
  • Substitute the assumed particular solution into the differential equation and solve for the unknown coefficients
  • The resulting particular solution, when added to the complementary solution, gives the general solution to the nonhomogeneous system

Variation of Parameters

  • The variation of parameters method is a more general approach that can be used for any form of the inhomogeneous term
  • Start by finding the complementary solution to the corresponding homogeneous system
  • Assume a particular solution that is a linear combination of the solutions to the homogeneous system, with the coefficients being functions of the independent variable (usually time $t$)
  • Substitute the assumed particular solution into the differential equation and solve for the unknown functions
  • Integrate the resulting equations to find the particular solution
  • The particular solution, when added to the complementary solution, provides the general solution to the nonhomogeneous system

Forced Oscillations and Resonance

Forced Oscillations

  • Forced oscillations occur when an external force or input (the inhomogeneous term) acts on an oscillating system
  • The external force can have a different frequency than the natural frequency of the system
  • The system's response depends on the frequency and amplitude of the external force
  • The steady-state solution to a forced oscillation system consists of two parts:
    • The transient solution, which depends on the initial conditions and decays over time
    • The steady-state solution, which oscillates at the same frequency as the external force

Resonance

  • Resonance occurs when the frequency of the external force is close to or equal to the natural frequency of the system
  • At resonance, the amplitude of the steady-state solution becomes very large, even for small external forces
  • Resonance can lead to significant amplification of the system's oscillations and potentially cause damage or failure (bridges collapsing due to wind or earthquakes)
  • To avoid resonance, systems can be designed with damping or by ensuring that the external force frequencies are far from the natural frequencies of the system (shock absorbers in vehicles, tuned mass dampers in buildings)