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MIT 18.03 - Ordinary Differential Equations & Laplace Transforms

Master MIT's foundational differential equations with this high-yield flashcard deck. Dive into first-order ODEs, linear systems, and powerful Laplace transform methods to conquer complex mathematical problems.

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(24 cards)

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#1
Term
What is the general form of a second-order linear homogeneous ODE with constant coefficients?
Definition
The general form is , where are constants and .
#2
Term
What is an exact differential equation?
Definition
A first-order ODE is exact if rac{\partial M}{\partial y} = rac{\partial N}{\partial x}. The solution is given by , where rac{\partial F}{\partial x} = M and rac{\partial F}{\partial y} = N.
#3
Term
What is an Ordinary Differential Equation (ODE)?
Definition
An Ordinary Differential Equation (ODE) is an equation involving an unknown function of a single independent variable and its derivatives with respect to that variable. For example, rac{dy}{dx} = xy.
#4
Term
How is the order of an ODE determined?
Definition
The order of an ODE is determined by the highest derivative present in the equation. For example, is a third-order ODE.
#5
Term
What is the general form of a first-order linear ODE?
Definition
The general form of a first-order linear ODE is rac{dy}{dx} + P(x)y = Q(x), where and are continuous functions of .
#6
Term
How do you solve a first-order linear ODE using an integrating factor?
Definition
To solve rac{dy}{dx} + P(x)y = Q(x), first calculate the integrating factor . Then, multiply the entire ODE by to get rac{d}{dx}[I(x)y] = I(x)Q(x). Integrate both sides with respect to to find : , so y = rac{1}{I(x)}\left(\int I(x)Q(x)dx + C ight).
#7
Term
What is a separable ODE and how is it solved?
Definition
A separable ODE is a first-order ODE that can be written in the form rac{dy}{dx} = g(x)h(y). It is solved by separating the variables and integrating: \int rac{1}{h(y)}dy = \int g(x)dx.
#8
Term
How is the characteristic equation derived for ?
Definition
Assuming a solution of the form , we substitute and into the ODE. This yields . Dividing by (which is never zero), we get the characteristic equation: .
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