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ordinary differential equation (ODE)
derivatives WRT only ONE independent variable
partial differential equation (PDE)
several derivatives WRT >1 independent variable
∇2 (Laplacian operator) indicates PDE
usually indicated by ∂x (partial diff) if x is a function that has more than 1 variable as inputs
order
the number of the highest derivative in a function
order can be measured in both ODE & PDE
linear
the unknown variable & its derivatives appear
at power 0 or 1
not multiplied by each other, but maybe multiplied with another function x
not inside nonlinear functions (functions whose Taylor expansion has higher powers, like sin)
can be ODE or PDE
linear homogeneous
all terms include the unknown variable; = 0
linear inhomogeneous
not all terms include the unknown; = constant or other function
Solution to y’ = ay
y = Aeax
Solution to y’ + a2y = 0
y = Aeax + Be-ax
y’ - a2y = 0
y = A cos(ax) + B sin(ax)
explicit solution
unknown function is directly in terms of independent variables
y = f(x)
implicit solution
unknown function is not directly in terms of independent variables
F(x,y) = 0
general vs specific solution
general
all solutions for differential equation
usually contains arbitrary constants
specific
follows initial conditions
no arbitrary unknown constants
integrating factor method
for first order linear ODEs of the form:
y’ + py = q
multiply by u = e^(int p dt)
reverse product rule
technique for solving 1st order linear ODEs when one side of the equation is the derivative of a product
variation of parameters
technique for solving inhomogeneous 1st order ODEs when homogeneous solution is easier to solve
convert to homogeneous form
compute y and y’ in terms of f(x) which takes C’s place
substitute y and y’ into og inhomogeneous equation
integrate both sides WRT s, usually f(x) is isolateable by now
substitute f(x) back into yh(x)
singular solution
solution to a differential equation that cannot be obtained by plugging in values of constants from the general solution — but still satisfies the equation
exact equation
equation that can be written in the form of
dψ = Mdx + Ndy = 0
Solving an exact equation steps
Check My = Nx
Integrate M WRT x and add h(y)
Differentiate WRT y
Set equal to N(x,y)
Integrate h’(y)
Substitute h(y) back into original equation for potential function
Solving exact equation when M & N are not exact
Multiply Mdx + Ndy = 0 by μ
My = μ’M + μM’ WRT y
Nx = μ’N + μN’ WRT x
Set My = Nx
Assume μ = μ(x), and thus set μy = 0
Find μ(x), then multiply the original equation by μ(x) to make it exact
Substitution when dy/dx = F(y/x)
Use v(x) = y/x, y = xv, y’ = v + xvb’
Separate new equation by term
Integrate both sides
Substitute y back in for v
Isolate y