| Line 5: |
Line 5: |
| | :<math>M(t,y) + N(t,y)y' = 0\,</math> or <math>M(t,y) dt + N(t,y) dy = 0\,</math> | | :<math>M(t,y) + N(t,y)y' = 0\,</math> or <math>M(t,y) dt + N(t,y) dy = 0\,</math> |
| | | | |
| − | To find the solution of this equation, we assume that the solution is φ = constant. This means that:
| + | Before we begin solving it, we must first check that the equation is exact. This means that: |
| − | <math>\frac{\partial \phi}{\partial t} = M</math> and <math>\frac{\partial \phi}{\partial y} = N</math>, since <math>(\frac{\partial \phi}{\partial t}) dt + (\frac{\partial \phi}{\partial y}) dy = 0</math>
| |
| | | | |
| − | φ is found by integrating M and N: | + | <math>\frac{\partial M}{\partial y} = \frac{\partial N}{\partial t}</math> |
| − | :<math>\phi(t, y) = \int_0^t M(s, 0) ds + \int_0^y N(t, s) ds</math>
| + | |
| | + | To find the solution of this equation, we assume that the solution is φ = constant. We can re-write a different form of this equation by substituting <math>\frac{\partial \phi}{\partial t} = M</math> and <math>\frac{\partial \phi}{\partial y} = N</math>. This yields <math>(\frac{\partial \phi}{\partial t}) dt + (\frac{\partial \phi}{\partial y}) dy = 0</math>, which makes sense. |
| | + | |
| | + | to find φ, we integrate M with respect to t and N with respect to y. This will give us two different equations. To find φ , we |
| | | | |
| | Go through the example to find φ by integrating, then check that | | Go through the example to find φ by integrating, then check that |
| Line 17: |
Line 19: |
| | and that any function φ = some constant, when turned into the corresponding dy/dt, satisfies the original equation. Be sure to emphasize that one must check first that | | and that any function φ = some constant, when turned into the corresponding dy/dt, satisfies the original equation. Be sure to emphasize that one must check first that |
| | :<math>\frac{\partial M}{\partial y} = \frac{\partial N}{\partial t}</math> | | :<math>\frac{\partial M}{\partial y} = \frac{\partial N}{\partial t}</math> |
| − | (That's the condition for "exactness" of the differential form M dt + N dy.)
| |
| − |
| |
| − |
| |
| − | where <math>\frac{\partial M}{\partial y} = \frac{\partial N}{\partial t}</math>.
| |
| | | | |
| | To find <math>y</math>, first set <math>M = \frac{\partial \phi}{\partial t}</math> and <math>N = \frac{\partial \phi}{\partial y}</math>. Then manipulate to get <math>M \partial t = \partial \phi</math> and <math>N \partial y = \partial \phi</math>. Integrate both sides, compare the results for <math>\phi</math>, and combine the terms into one equation (for terms that show up in both expressions, only write once in the combined expression.) To solve the expression for <math>y</math>, plug into the quadratic formula. | | To find <math>y</math>, first set <math>M = \frac{\partial \phi}{\partial t}</math> and <math>N = \frac{\partial \phi}{\partial y}</math>. Then manipulate to get <math>M \partial t = \partial \phi</math> and <math>N \partial y = \partial \phi</math>. Integrate both sides, compare the results for <math>\phi</math>, and combine the terms into one equation (for terms that show up in both expressions, only write once in the combined expression.) To solve the expression for <math>y</math>, plug into the quadratic formula. |