Second-order homogeneous differential equations
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“Second-order homogeneous differential equations” involve equations that equate to zero and include second-order derivatives.
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To differentiate an equation means to find the rate at which the original function changes. In the case of second-order derivatives, you’re finding the rate at which the rate changes.
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These types of equations are important in various fields, notably in physics where they can describe motion or other physical properties changing with respect to time.
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They have a general form, often written as ay’’ + by’ + c*y = 0. Here, ‘y’ is the dependent variable, ‘a’, ‘b’ and ‘c’ are constants, and y’’ is the second derivative of y with respect to the independent variable, while y’ is the first derivative of y.
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The solutions to these second-order homogeneous differential equations is often searched in the form of y = e^(r*x). By substituting this solution form into the differential equation, a characteristic equation arises.
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The characteristic equation is a quadratic equation of the form ar^2 + br + c = 0 where roots determine the nature of the solution.
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There are three possible types of solutions based on the discriminant (B^2 - 4AC) values in the characteristic equation: Real and different roots, Real and same roots, and Complex roots.
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For real and different roots, the general solution will be y = Ae^(r1x) + Be^(r2x), where A and B are arbitrary constants and r1, r2 are the roots of the characteristic equation.
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For real and same roots (repeated root), the general solution will be y = (A + B * x) e^(r * x).
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For complex roots, the general solution will be y = e^(ax)(Ccos(bx) + D*sin(bx)), where ‘a’ is the real part and ‘b’ is the imaginary part.
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To further define the exact solution, initial conditions (i.e, values of the original function and its first derivative at specific points) are normally given.