Skip to content

Introduction and Classification

A differential equation (DE) is an equation involving an unknown function and its derivatives. An ordinary differential equation (ODE) involves a function of one variable and its ordinary Derivatives. A partial differential equation (PDE) involves a function of several variables and Its partial derivatives.

An ODE is:

  • Ordinary vs. partial: depends on whether partial derivatives appear.
  • Order: the highest derivative that appears.
  • Linear vs. nonlinear: linear if the unknown function and its derivatives appear linearly.
  • Homogeneous vs. nonhomogeneous: for linear ODEs, homogeneous if the forcing term is zero.

An initial value problem (IVP) specifies the value of the function (and possibly its Derivatives) at a single point. A boundary value problem (BVP) specifies conditions at two or More points.

Differential equations arise throughout the natural sciences. A few canonical examples:

  1. Newton”s law of cooling. The temperature T(t)T(t) of a body in a medium at temperature TmT_m satisfies dTdt=k(TTm)\frac{dT}{dt} = -k(T - T_m)A first-order linear ODE.

  2. Harmonic oscillator. A mass on a spring with damping obeys md2xdt2+cdxdt+kx=F(t)m\frac{d^2 x}{dt^2} + c\frac{dx}{dt} + kx = F(t)A second-order linear ODE.

  3. Logistic population growth. dPdt=rP(1PK)\frac{dP}{dt} = rP\left(1 - \frac{P}{K}\right)A first-order nonlinear (Bernoulli) ODE.

  4. Lotka-Volterra predator-prey model. dxdt=x(αβy)\frac{dx}{dt} = x(\alpha - \beta y), dydt=y(γ+δx)\frac{dy}{dt} = y(-\gamma + \delta x)A coupled nonlinear system.

  5. RC circuit. The charge q(t)q(t) on a capacitor satisfies Rdqdt+qC=V(t)R\frac{dq}{dt} + \frac{q}{C} = V(t) a first-order linear ODE.

  6. Heat equation. The temperature u(x,t)u(x, t) in a rod satisfies ut=α2uxxu_t = \alpha^2 u_{xx}A second-order linear PDE.

  7. Wave equation. The displacement u(x,t)u(x, t) of a string satisfies utt=c2uxxu_{tt} = c^2 u_{xx}A second-order linear PDE.

  8. Laplace’s equation. The steady-state temperature satisfies uxx+uyy=0u_{xx} + u_{yy} = 0A second-order linear PDE.

Differential Equations
├── ODE (one independent variable)
│ ├── By order
│ │ ├── First-order: y' = f(x, y)
│ │ ├── Second-order: y'' = f(x, y, y')
│ │ └── n-th order: y^(n) = f(x, y, ..., y^(n-1))
│ ├── By linearity
│ │ ├── Linear: a_n(x)y^(n) + ... + a_0(x)y = g(x)
│ │ │ ├── Homogeneous (g = 0)
│ │ │ └── Nonhomogeneous (g ≠ 0)
│ │ └── Nonlinear (y or derivatives appear nonlinearly)
│ └── By coefficients
│ ├── Constant coefficient
│ └── Variable coefficient
└── PDE (multiple independent variables)
├── Elliptic: B² - 4AC < 0 (e.g., Laplace)
├── Parabolic: B² - 4AC = 0 (e.g., Heat)
└── Hyperbolic: B² - 4AC > 0 (e.g., Wave)

Problem. Classify each equation by order, linearity, and homogeneity (if linear).

(a) y+3y+2y=sinxy'' + 3y' + 2y = \sin x

(b) (y)2+y=0(y')^2 + y = 0

(c) x2y+xy+(x21)y=0x^2 y'' + xy' + (x^2 - 1)y = 0

(d) 2ux2+2uy2=0\frac{\partial^2 u}{\partial x^2} + \frac{\partial^2 u}{\partial y^2} = 0

Solution

(a) Second-order, linear, nonhomogeneous (forcing term sinx0\sin x \neq 0).

(b) First-order, nonlinear (the term (y)2(y')^2 is nonlinear in yy').

(c) Second-order, linear, homogeneous. This is Bessel’s equation of order 1.

(d) Second-order PDE, linear, homogeneous. This is Laplace’s equation; A=1A = 1, C=1C = 1, B=0B = 0 So B24AC=4<0B^2 - 4AC = -4 \lt 0 (elliptic). \blacksquare

  • Confusing order with degree. The order of an ODE is the highest derivative, not the highest power of yy or yy'.
  • Misidentifying linearity. A term like yyyy' or (y)2(y')^2 makes an ODE nonlinear, even if each derivative appears only once.
  • Mixing up IVP and BVP. An IVP specifies conditions at a single point; a BVP specifies conditions at two or more distinct points.
  • Assuming superposition for nonlinear equations. The superposition principle applies only to linear homogeneous ODEs.
EquationOrderLinear?Homogeneous?Type
y+3y=0y' + 3y = 01YesYesLinear, constant coeff.
y+y=sinty'' + y = \sin t2YesNoLinear, constant coeff.
y=y2y' = y^21NoNonlinear
x2y+xy+(x2n2)y=0x^2 y'' + xy' + (x^2-n^2)y = 02YesYesBessel’s equation
ut=α2uxxu_t = \alpha^2 u_{xx}2YesYesHeat equation (PDE)

Differential equations describe how things change. An ODE relates a function to its derivatives, capturing the idea that the rate of change depends on the current state. A first-order ODE like y=f(x,y)y' = f(x, y) says the slope at each point is determined by the coordinates. Linearity means the superposition principle applies: sums of solutions are solutions. The order is the number of times you differentiate — a second-order equation involves acceleration, as in Newton’s second law. Homogeneous equations have no external forcing, so the zero solution works. Classification guides the solution method: constant-coefficient equations use characteristic equations, while variable-coefficient equations may require series or numerical methods.

  • Engineering: Electrical circuit analysis (RLC circuits) and control systems rely on linear ODEs with constant coefficients.
  • Biology: Epidemiological models (SIR equations) and population dynamics use nonlinear systems of ODEs.
  • Physics: Newtonian mechanics, quantum mechanics (Schrödinger equation), and general relativity (Einstein field equations) are formulated as differential equations.
  • Economics: Black-Scholes equation for option pricing is a PDE; macroeconomic growth models use ODE systems.

This section provides detailed coverage of advanced concepts, including full derivations, proofs, and extended examples.

Complete mathematical derivations and proofs are provided where appropriate. Each step is explained to ensure understanding of the underlying reasoning.

Advanced examples demonstrate the application of concepts to complex problems. These examples go beyond standard exam questions to develop deeper understanding.

This material connects to current research and advanced applications in the field. Understanding these connections provides context for the study material.

Ensure you have mastered the prerequisite material before attempting this advanced content.

This section provides detailed coverage of advanced concepts, including full derivations, proofs, and extended examples.

Complete mathematical derivations and proofs are provided where appropriate. Each step is explained to ensure understanding of the underlying reasoning.

Advanced examples demonstrate the application of concepts to complex problems. These examples go beyond standard exam questions to develop deeper understanding.

This material connects to current research and advanced applications in the field. Understanding these connections provides context for the study material.

Ensure you have mastered the prerequisite material before attempting this advanced content.