Difference between revisions of "Solutions of Differential Equations"

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* <math> y' = 2x </math>. Through simple integration, we can calculate the general solution of this equation to be <math>y = x^2 + C</math>, where C is an arbitrary constant.
 
* <math> y' = 2x </math>. Through simple integration, we can calculate the general solution of this equation to be <math>y = x^2 + C</math>, where C is an arbitrary constant.
 
* <math> y' - y = 0 </math>. The G.S. is <math> y = Ce^{x} </math>. <math> y' = Ce^{x} </math>, so <math> y' - y = 0 \to Ce^{x} - Ce^{x} = 0</math>, so this solution satisfies the relationship for all arbitrary constants C.
 
* <math> y' - y = 0 </math>. The G.S. is <math> y = Ce^{x} </math>. <math> y' = Ce^{x} </math>, so <math> y' - y = 0 \to Ce^{x} - Ce^{x} = 0</math>, so this solution satisfies the relationship for all arbitrary constants C.
* <math> y' + y - 2 = 0 </math>. The G.S. is <math> y = Ce^{-x} + 2 </math>. <math> y' = -Ce^{-x} </math>, so <math> 0 = y' + y - 2 </math> becomes <math> 0 = -Ce^{-x} + Ce^{-x} + 2 - 2 = 0 </math>.
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* <math> y'' + y' - 2y = 0 </math>. The G.S. is <math> y = Ce^{x} + De^{-2x} </math>. <math> y' = Ce^{x} - 2De^{-2x} </math> and <math> y'' = Ce^{x} + 4De^{-2x} </math>, so <math> 0 = y'' + y' - 2y </math> becomes <math> 0 = Ce^{x} + 4De^{-2x} + Ce^{x} - 2De^{-2x} - 2(Ce^{x} + De^{-2x}) = Ce^{x} + Ce^{x} - 2Ce^{x} + 4De^{-2x} - 2De^{-2x} - 2De^{-2x}) = 0 </math>.
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The particular solution of a differential equation can be solved if we have enough points to solve for the arbitrary constants.
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Examples:
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* <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>.
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* <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>.
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* <math> y'' + y' - 2y = 0 </math>. The G.S. is <math> y = Ce^{x} + De^{-2x} </math>. <math> y' = Ce^{x} - 2De^{-2x} </math> and <math> y'' = Ce^{x} + 4De^{-2x} </math>, so <math> 0 = y'' + y' - 2y </math> becomes <math> 0 = Ce^{x} + 4De^{-2x} + Ce^{x} - 2De^{-2x} - 2(Ce^{x} + De^{-2x}) = Ce^{x} + Ce^{x} - 2Ce^{x} + 4De^{-2x} - 2De^{-2x} - 2De^{-2x}) = 0 </math>.
  
  

Revision as of 19:47, 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 .
  • . The G.S. is . and , so becomes .


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