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Key Terms

boundary conditions
the conditions that give the state of a system at different times, such as the position of a spring-mass system at two different times
boundary-value problem
a differential equation with associated boundary conditions
characteristic equation
the equation aλ2+bλ+c=0aλ2+bλ+c=0 for the differential equation ay+by+cy=0ay+by+cy=0
complementary equation
for the nonhomogeneous linear differential equation
a2(x)y+a1(x)y+a0(x)y=r(x),a2(x)y+a1(x)y+a0(x)y=r(x),

the associated homogeneous equation, called the complementary equation, is
a2(x)y+a1(x)y+a0(x)y=0a2(x)y+a1(x)y+a0(x)y=0
homogeneous linear equation
a second-order differential equation that can be written in the form a2(x)y+a1(x)y+a0(x)y=r(x),a2(x)y+a1(x)y+a0(x)y=r(x), but r(x)=0r(x)=0 for every value of xx
linearly dependent
a set of functions f1(x),f2(x),…,fn(x)f1(x),f2(x),…,fn(x) for which there are constants c1,c2,…cn,c1,c2,…cn, not all zero, such that c1f1(x)+c2f2(x)++cnfn(x)=0c1f1(x)+c2f2(x)++cnfn(x)=0 for all x in the interval of interest
linearly independent
a set of functions f1(x),f2(x),…,fn(x)f1(x),f2(x),…,fn(x) for which there are no constants c1,c2,…cn,c1,c2,…cn, such that c1f1(x)+c2f2(x)++cnfn(x)=0c1f1(x)+c2f2(x)++cnfn(x)=0 for all x in the interval of interest
method of undetermined coefficients
a method that involves making a guess about the form of the particular solution, then solving for the coefficients in the guess
method of variation of parameters
a method that involves looking for particular solutions in the form yp(x)=u(x)y1(x)+v(x)y2(x),yp(x)=u(x)y1(x)+v(x)y2(x), where y1y1 and y2y2 are linearly independent solutions to the complementary equations, and then solving a system of equations to find u(x)u(x) and v(x)v(x)
nonhomogeneous linear equation
a second-order differential equation that can be written in the form a2(x)y+a1(x)y+a0(x)y=r(x),a2(x)y+a1(x)y+a0(x)y=r(x), but r(x)0r(x)0 for some value of xx
particular solution
a solution yp(x)yp(x) of a differential equation that contains no arbitrary constants
RLC series circuit
a complete electrical path consisting of a resistor, an inductor, and a capacitor; a second-order, constant-coefficient differential equation can be used to model the charge on the capacitor in an RLC series circuit
simple harmonic motion
motion described by the equation x(t)=c1cos(ωt)+c2sin(ωt),x(t)=c1cos(ωt)+c2sin(ωt), as exhibited by an undamped spring-mass system in which the mass continues to oscillate indefinitely
steady-state solution
a solution to a nonhomogeneous differential equation related to the forcing function; in the long term, the solution approaches the steady-state solution
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