Difference between revisions of "Solutions of Differential Equations"

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Examples:
 
Examples:
 
* <math> y' = 2x </math>, <math> y(2) = 0 </math>. With this point and the general solution <math>y = x^2 + C</math>, we can calculate the constant C to be -4. Thus the particular solution is <math>y = x^2 - 4</math>.
 
* <math> y' = 2x </math>, <math> y(2) = 0 </math>. With this point and the general solution <math>y = x^2 + C</math>, we can calculate the constant C to be -4. Thus the particular solution is <math>y = x^2 - 4</math>.
* <math> y' - y = 0 </math>, <math> y(0) = 3 </math>. <math> 3 = Ce^{0} = C</math>, so the particular solution is <math> y = 3e^{x} </math>.
+
* <math> y' - y = 0 </math>, <math> y(0) = 3 </math>. <math> 3 = Ce^{0} \implies C = 3</math>, so the particular solution is <math> y = 3e^{x} </math>.
 
* <math> y'' + y' - 2y = 0 </math>, <math> y(0) = 2 </math>, <math> y'(0) = -1 </math>. So, <math> 2 = Ce^{0} + De^{0} = C + D </math> and <math> -1 = Ce^{0} - 2De^{0} = C - 2D</math>. Thus C = 1 and D = 1, and the particular solution is <math> y = e^{x} + e^{-2x} </math>.
 
* <math> y'' + y' - 2y = 0 </math>, <math> y(0) = 2 </math>, <math> y'(0) = -1 </math>. So, <math> 2 = Ce^{0} + De^{0} = C + D </math> and <math> -1 = Ce^{0} - 2De^{0} = C - 2D</math>. Thus C = 1 and D = 1, and the particular solution is <math> y = e^{x} + e^{-2x} </math>.
  

Revision as of 19:54, 17 September 2021

A solution of a differential equation is an expression of the dependent variable that satisfies the relation established in the differential equation. For example, the solution of will be some equation y = f(x) such that y and its first derivative, y', satisfy the relation . The general solution of a differential equation will have one or more arbitrary constants, depending on the order of the original differential equation (the solution of a first order diff. eq. will have one arbitrary constant, a second order one will have two, etc.).

Examples:

  • . Through simple integration, we can calculate the general solution of this equation to be , where C is an arbitrary constant.
  • . The G.S. is . , so , so this solution satisfies the relationship for all arbitrary constants C.
  • . The G.S. is . and , so becomes .

The particular solution of a differential equation can be solved if we have enough points to solve for the arbitrary constants.

Examples:

  • , . With this point and the general solution , we can calculate the constant C to be -4. Thus the particular solution is .
  • , . , so the particular solution is .
  • , , . So, and . Thus C = 1 and D = 1, and the particular solution is .

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