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Differential Equations and Vector Calculus

First-Order Differential Equations

Physics I 224 words Free to read

First-Order ODEs

A first-order differential equation involves only first derivatives and has the general form:

dydx=f(x,y)\frac{dy}{dx} = f(x, y)

Separable equations occur when f(x,y)=g(x)h(y)f(x,y) = g(x)h(y). Rearrange and integrate both sides:

dyh(y)=g(x)dx\int \frac{dy}{h(y)} = \int g(x)\,dx

Linear first-order equations match the standard form y+P(x)y=Q(x)y' + P(x)y = Q(x). Solve them using the integrating factor μ\mu:

μ=ePdx,y=1μμQdx\mu = e^{\int P\,dx}, \quad y = \frac{1}{\mu}\int \mu\,Q\,dx

Worked Example: Radioactive decay is modeled by dNdt=λN\frac{dN}{dt} = -\lambda N. Separating variables yields the solution N=N0eλtN = N_0 e^{-\lambda t}, showing exponential decrease over time.

Core Types & Pitfalls

First-order equations fall into four main categories, each requiring a specific solution strategy:

TypeStandard FormSolution Method
Separabley=g(x)h(y)y' = g(x)h(y)Separate variables
Lineary+Py=Qy' + Py = QIntegrating factor
ExactMdx+Ndy=0M\,dx + N\,dy = 0Potential function
Bernoulliy+Py=Qyny' + Py = Qy^nSubstitution v=y1nv = y^{1-n}

Physics Link: Newton's law of cooling, dTdt=k(TTenv)\frac{dT}{dt} = -k(T - T_{\text{env}}), is a linear first-order ODE governing thermal equilibrium.

Common Pitfall: The general solution of a first-order ODE requires an arbitrary constant. Forgetting +C (or ignoring initial conditions) yields a specific solution rather than the complete solution required for your problem.

Placeholder: First-Order Differential Equations

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Differential Equations and Vector Calculus