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integrate dy/dx |
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| Aug27-09, 03:57 PM | #1 |
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integrate dy/dx
can some one explain to me how the set of all solutions for dy/dx = 3y
is. y= Ce^3x 1. The problem statement, all variables and given/known data 2. Relevant equations 3. The attempt at a solution |
| Aug27-09, 04:18 PM | #2 |
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Recognitions:
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Simply separate the variables.
[tex] \begin{align*} \frac{dy}{dx} & = 3y \\ \frac 1 y \frac dy dx & = 3 \\ \int \left(\frac 1 y\right) \left(\frac{dy}{dx}\right) \, dx & =\int 3 \, dx \end{align*} [/tex] You should be able to finish from here. |
| Aug27-09, 04:20 PM | #3 |
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Recognitions:
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Try rearranging your equation to get it in the form f(y)dy=g(x) dx. Then integrate both sides.
This type of differential equation technique is called 'separation of variables' |
| Aug27-09, 04:23 PM | #4 |
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integrate dy/dx
i got y= e^3x + e^c
how does that become y= Ce^3x |
| Aug27-09, 04:37 PM | #5 |
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Mentor
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Instead of e3x + eC, you should have gotten e3x + C = e3xeC = C' e3x
(Here, C' = eC. After all, eC is just a constant.) |
| Aug27-09, 04:59 PM | #6 |
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o ok thanks got it.
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| Aug27-09, 05:19 PM | #7 |
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this is variable separable. c is constant, then you can make it In c so that when using the e function, In c become only c.
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| Aug27-09, 06:03 PM | #8 |
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Mentor
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| Aug27-09, 07:47 PM | #9 |
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Here's a proof of the general case that I got from Courant's Introduction to Calculus and Analysis. This is one of my favourite proofs:
"If a function y = f(x) satisfies an equation of the form [tex] y' = \alpha y [/tex] where [tex] \alpha [/tex] is a constant, then y has the form [tex] y = f(x) = ce^{\alpha x} [/tex] where c is also a consant; conversely, every function of the form [tex] ce^{\alpha x} [/tex] satisfies the equation [tex] y' = \alpha y [/tex]. It is clear that [tex] y = ce^{\alpha x} [/tex] satisfies this equation for any arbitrary constant c. Conversely, no other function satisfies the differential equation [tex] y' - \alpha y = = [/tex]. For if y is such a function, we consider the function [tex] u = ye^{-\alpha x} [/tex]. We then have [tex] u' = y'e^{-\alpha x} - \alpha y e^{-\alpha x} = e^{-\alpha x}(y' - \alpha y}) .[/tex] However, the right-hand side vanishes, since we have assumed that [tex] y' = \alpha y [/tex]; hence [tex] u' = 0 [/tex] so that u is a constant c and [tex] y = ce^{\alpha x} [/tex] as we wished to prove." |
| Aug28-09, 05:31 AM | #10 |
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yes its ln but I type In. Sorry.
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