Solution:Second Order Linear Non-Homogenous ODEs in Physics

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SUMMARY

Second order linear non-homogeneous ordinary differential equations (ODEs) are crucial in various physics applications, particularly in electric circuits and mechanics. In RLC circuits, the governing equation is given by \(\frac{q}{C}+R\frac{dq}{dt}+L\frac{d^2q}{dt^2}=V(t)\), where \(q(t)\) represents the charge over time. In mechanics, the damped harmonic oscillator is described by the equation \(m\frac{d^2x}{dt^2}+c\frac{dx}{dt}+kx=F(t)\), with \(x(t)\) denoting the displacement of the mass. These equations model dynamic systems influenced by external forces and are foundational in understanding physical phenomena.

PREREQUISITES
  • Understanding of second order linear ordinary differential equations
  • Familiarity with electric circuit components: resistors, capacitors, and inductors
  • Knowledge of mechanical systems, specifically damped harmonic oscillators
  • Basic calculus, particularly differentiation and integration techniques
NEXT STEPS
  • Study the application of Laplace transforms in solving second order linear ODEs
  • Explore the concept of forced oscillations in mechanical systems
  • Investigate the role of damping in oscillatory motion
  • Learn about the transient and steady-state responses in RLC circuits
USEFUL FOR

Students and professionals in physics, electrical engineering, and mechanical engineering who are looking to deepen their understanding of dynamic systems and their mathematical modeling through differential equations.

Dimitris Papadim
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Hello, could someone please give me some examples of where order linear non homogenous ordinary differential equations are used in physics[emoji4]
 
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They have many applications in almost all areas of physics.

For example in physics-electric circuits the differential equation that governs the behaviour of a RLC circuit with a resistor of ohmic resistance R, Capacitor of capacitance C and inductor of inductance L, all in series, which is driven by a voltage source V(t) is given by ##\frac{q}{C}+R\frac{dq}{dt}+L\frac{d^2q}{dt^2}=V(t)##. q(t) is the charge of the capacitor C at time t.

Another example in physics-mechanics, the damped harmonic oscillator with mass m, spring constant k, and damping coefficient c, that is driven by an external force F(t) follows the 2nd order linear ordinary differential equation:
##m\frac{d^2x}{dt^2}+c\frac{dx}{dt}+kx=F(t)##. x(t) is the displacement of mass m at time t.
 
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