Solving Initial Value Problem: \(\ln(t)+t^2y^2-\sin(y)=\pi^2\)

[alane1994]

Ok, I have a practice exam... My professor gave out a copy with worked out examples. There is one where I don't get his logic at all. I was wondering if you guys could explain it to me?\(\displaystyle (\frac{1}{t}+2y^2t)dt+(2yt^2-\cos(y))dy=0\)

First, he put \(\text{Assume t>0}\)
?

\(\displaystyle \text{Since} \frac{\partial}{\partial y}(\frac{1}{t}+2y^2t)=4yt=\frac{\partial}{\partial t}(2yt^2-\cos(y))\)

\(\displaystyle F(t,y)=\int (\frac{1}{t}+2y^2t)dt=\ln(t)+y^2t^2+f(y)\)
\(\displaystyle ~~~~~~~~~~~=\int (2yt^2-\cos(y))dy=y^2ts-\sin(y)+g(t)\)

From those (not sure how to do two lines into right brace).

\(\ln(t)+t^2y^2-\sin(y)=C\)
\(y(1)=\pi\)
\(0+\pi^2-0=C\)

\(\therefore \ln(t)+t^2+y^2-\sin(y)=\pi^2\)

 

[chisigma]

Re: Ivp

Ok, I have a practice exam... My professor gave out a copy with worked out examples. There is one where I don't get his logic at all. I was wondering if you guys could explain it to me?\(\displaystyle (\frac{1}{t}+2y^2t)dt+(2yt^2-\cos(y))dy=0\)

First, he put \(\text{Assume t>0}\)
?

\(\displaystyle \text{Since} \frac{\partial}{\partial y}(\frac{1}{t}+2y^2t)=4yt=\frac{\partial}{\partial t}(2yt^2-\cos(y))\)

\(\displaystyle F(t,y)=\int (\frac{1}{t}+2y^2t)dt=\ln(t)+y^2t^2+f(y)\)
\(\displaystyle ~~~~~~~~~~~=\int (2yt^2-\cos(y))dy=y^2ts-\sin(y)+g(t)\)

From those (not sure how to do two lines into left brace).

\(\ln(t)+t^2y^2-\sin(y)=C\)
\(y(1)=\pi\)
\(0+\pi^2-0=C\)

\(\therefore \ln(t)+t^2+y^2-\sin(y)=\pi^2\)

An ODE written in the form...$\displaystyle A (t,y)\ dt + B(t,y)\ dy = 0\ (1)$

... where $\displaystyle \frac{\partial A}{\partial y}= \frac{\partial B}{\partial t}$ is called 'exact differential' and its solution, with initial condition $y(t_{0})= y_{0}$ is... $\displaystyle \int_{t_{0}}^{t} A(u,y)\ du + \int_{y_{0}}^{y} B(t_{0},v)\ dv = c\ (2)$

In Your case is $\displaystyle A(t,y) = \frac{1}{t} + 2\ y^{2}\ t$ and $\displaystyle B (t,y) = 2\ y\ t^{2} - \cos y$ so that $\displaystyle \frac{\partial A}{\partial y} = \frac{\partial B}{\partial t}$ and You have an exact differential. The general solution is given from (2)...

$\displaystyle \int_{t_{0}}^{t} (\frac{1}{u} + 2\ u\ y^{2})\ du + \int_{y_{0}}^{y} (2\ t_{0}^{2}\ v - \cos v)\ dv= c\ (3)$

... and the integration of (3) is left to You...

Kind regards

$\chi$ $\sigma$

 

[alane1994]

Where did the the

\(y^2ts\)

come from?

How did terms cancel like that? It seems like they shouldn't.

 

[HallsofIvy]

Re: Ivp

This is a pretty standard "exact differential" problem. First, the "Assume t> 0" is to avoid t= 0 which, because of the "1/t", would cause trouble. Of course there would be another solution if we were to "assume t< 0".

(I just noticed that I have used "x, y" where you have "t, y". Assume my "x" is your "t".)

If F(x, y) is a differentiable function of x and y, then its differential is \frac{\partial F}{\partial x}dx+ \frac{\partial F}{\partial y}dy. As long as those partial derivatives are smooth, we must have the "mixed derivatives" the same: \frac{\partial^2 F}{\partial x\partial y}= \frac{\partial^2 F}{\partial y\partial x} (where the order of "\partial x" and "tex]\partial y[/tex]" indicates the order of differentiation).

Now, we can write "u(x,y)dx+ v(x,y)dy" which looks like a differential- but it may not be! (We would say it is not "exact".) If this were really a differential, We would have to have \frac{\partial F}{\partial x}=u and \frac{\partial F}{\partial y}= v then \frac{\partial^2 F}{\partial x\partial y}= \frac{\partial u}{\partial y}= \frac{\partial v}{\partial x}= \frac{\partial^2 F}{\partial y\partial x}.

That is what is called the "mixed partials test" and they are showing after "Since".

Because that is true, we know there exist some function, F(x,y) such that \frac{\partial F}{\partial x}= \frac{1}{x}+ 2y^2x. Integrating (with respect to x, treating y as a constant) F= ln(x)+ y^2x^2+ \phi(y). (Since we are treating y as a constant, the "constant of integration" may depend on y. That is the "\phi(y)" above.)

Now, differentiate F= ln(x)+ y^2x^2+ \phi(y) with respect to y: \frac{\partial F}{\partial y}= 2y^2x+ \frac{d\phi}{dy}. (Notice that the derivative of \phi is an ordinary derivative, not a partial derivative because \phi is a function of the single variable y.)

But we know, from the equation, \frac{\partial F}{\partial y}= 2yx^2- cos(y) so we must have 2y^2x+ \frac{d\phi}{dy}= 2yx^2- cos(y). Notice that the only terms involving x, 2yx^2, cancel! That had to happen because of the "mixed derivatives" condition. That leaves just \frac{d\phi}{dy}= -cos(y) so that \phi(y)= -sin(y)+ C (C really is a constant here) so that
F(x,y)= ln(x)+ y^2x^2- sin(y)+ C.

Since the differential equation was "dF= 0", F must be a constant: F(x,y)= ln(x)+ y^2x^2- sin(y)+C= c or just F(x, y)= ln(x)+ y^2x^2- sin(y)= C&#039; where I have combined the two constants: C'= c- C.

Dropping the "F", which was not part of the original equation, ln(x)+ y^2x^2- sin(y)= C.

(Replacing x with your t:
ln(t)+ y^2t^2- sin(y)= C.)

(I suspect the "y^2ts" was a typo. It should be just "y^2t".)

 

[alane1994]

Thank you guys very much! Makes a lot more sense now!