Solving a system of differential equations

JD_PM
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Summary:: We want to find explicit functions ##g(y,t)## and ##f(y,t)## satisfying the following system of differential equations.

I attached a very similar solved example.

Given the following system of differential equations (assuming ##y \neq 0##)

\begin{equation*}
-y\partial_t \left( g(y,t)\right) + f(y,t) = 0 \tag{1}
\end{equation*}

\begin{equation*}
y\partial_y \left( f(y,t)\right) -f(y,t) = 0 \tag{2}
\end{equation*}

\begin{equation*}
\frac{1}{y^2} \partial_t \left( f(y,t) \right) - \partial_y \left( \frac{1}{y^2} g(y,t) \right) - \frac{2}{y^3} g(y,t) = 0 \tag{3}
\end{equation*}

We want to find explicit functions ##g(y,t)## and ##f(y,t)## satisfying such system

Adding up ##(1)## and ##(2)##

\begin{equation*}
\partial_y \left( f(y,t)\right) - \partial_t \left( g(y,t)\right) = 0 \tag{4}
\end{equation*}

Equation ##(4)## is satisfied when

\begin{equation*}
f(y,t) = f(t), \ \ \ \ g(y,t) = g(y) \tag{5}
\end{equation*}

Plugging ##(5)## into ##(3)## yields

\begin{equation*}
\partial_t f(t) - \partial_y g(y) =0 \tag{6}
\end{equation*}

But I do not see how ##(6)## is going to lead us to get explicit functions for ##g(y,t)## and ##f(y,t)##.

I actually expect to get a second order differential equation out of working out the system, whose solution should provide us with explicit functions for ##g(y,t)## and ##f(y,t)##.

Could you please help me out to move forward?

Thank you! :biggrin:

PS: I attach an analogous example. I am following the same procedure to solve our original problem

3727329372932793823232.png
 
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on Phys.org
Is this homework ?

JD_PM said:
Equation (4) is satisfied when
But then (2) yields ##f = 0## !

By the way, (2) is easily solved for ##y## !
 
BvU said:
Is this homework ?

This is a system of differential equations I encountered while solving a specific problem I am solving to study for my exam. I guess you can call it homework 😅

BvU said:
But then (2) yields ##f = 0## !

By the way, (2) is easily solved for ##y## !

So if I am not mistaken you are suggesting not to add up ##(1)## and ##(2)## (?) How to proceed then? (sorry I am a bit rusty with differential equations).
 
JD_PM said:
I guess you can call it homework
Thread moved the schoolwork forums.
 
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JD_PM said:
sorry I am a bit rusty with differential equations
JD_PM said:
solving a specific problem I am solving to study for my exam
If (2) is already a stumbling block, and the 'analogous example' is typical for the exam, I fear with great fear ... :nb)

Compare
$$
\begin{equation*}

y\partial_y \left( f(y,t)\right) -f(y,t) = 0 \tag{2}

\end{equation*}
$$
with ##\ x \, f'(x) = f(x) \ ## :rolleyes:
 
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BvU said:
If (2) is already a stumbling block, and the 'analogous example' is typical for the exam, I fear with great fear ... :nb)

:oops:... let's not panic though!

BvU said:
Compare
$$
\begin{equation*}

y\partial_y \left( f(y,t)\right) -f(y,t) = 0 \tag{2}

\end{equation*}
$$
with ##\ x \, f'(x) = f(x) \ ## :rolleyes:

Thanks for the guidance! Let's start over

Focusing on ##(2)##, we deduce that it takes the form

\begin{equation*}
\partial_y \left( y \ f(x,y) \right) = 0
\end{equation*}

Where we need to impose

\begin{equation*}
\partial_y f(x,y) = - f(x,y)
\end{equation*}

The simplest function I can think of that satisfies this equation (setting the constant of integration equal to zero) is ##f(x,y) = e^{-\ln(y)}## i.e.

\begin{equation*}
\partial_y \left( y \ e^{-\ln(y)} \right) = e^{-\ln(y)} - y\left( \frac{1}{y} \right) \ e^{-\ln(y)} = \frac{1}{y} - \frac{1}{y} = 0
\end{equation*}

Plugging ##f(x,y) = e^{-\ln(y)}## into ##(1)## yields

\begin{equation*}
-y\partial_t \left( g(y,t) \right) + e^{-\ln(y)} = 0 \Rightarrow \partial_t \left( g(y,t) \right) = \frac{1}{y^2}
\end{equation*}

Thus (setting the constant of integration equal to zero) we get that ##g(x,y) = t/y^2##

But I have missed something as ##(3)## is not satisfied due to a factor of ##2## i.e.

\begin{equation*}
-\partial_y \left( \frac{t}{y^4} \right) - \frac{2t}{y^5} = \frac{2t}{y^5} \neq 0
\end{equation*}

What am I missing? I guess that I should impose a specific initial condition to get it done but I do not see it...
 
##\qquad##Funny, from $$
\begin{equation*}

\partial_y \left( y \; f(x,y) \right) = 0

\end{equation*}$$##\qquad## I get $$
\begin{equation*}
y\,\partial_y \left( f(y,t)\right) +f(y,t) = 0
\end{equation*}$$ where ##(2)## has a minus sign !

By the way, we physicists usually write ##e^{-\ln y} \ ## as ##\ \displaystyle{1\over y}\ ## :wink:

JD_PM said:
:oops:... let's not panic though!
That's the spirit !👍
 
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OK let's make it simpler

BvU said:
Compare
$$
\begin{equation*}

y\partial_y \left( f(y,t)\right) -f(y,t) = 0 \tag{2}

\end{equation*}
$$
with ##\ x \, f'(x) = f(x) \ ## :rolleyes:

So we see that ##f(y,t) = f(y) = e^{\ln y} = \frac{1}{y}## (so everyone is happy! haha) is a solution for ##(2)##

Then all we need to do is plugging it into ##(1)## and find ##g(y,t)## so that the following equation is satisfied

\begin{equation*}
\partial_t \left( g(y,t)\right) = \frac{1}{y^2}
\end{equation*}

Besides, ##g(y,t)## and ##f(y,t)## must be a solution for ##(3)## of course.

Thank you, I think I can get it done now (time to go back to study! 🤓).
 
JD_PM said:
so everyone is happy! haha
Hoho! Not yet! I'll let you know when I'm happy :wink:

As long as you write
JD_PM said:
So we see that ##f(y,t) = f(y) = e^{\ln y} = \frac{1}{y}##
I'm not happy by a long shot ! And the last bit ##e^{\ln y} = \frac{1}{y} ## is (probably :rolleyes:?) a typo, so that does not count.

##f(y,t)=f(y) ## is the one that is really irking me. We solve (we try to ...) for ##y## but that doesn't mean ##t## goes away.

We are still working on ##(2)## and are nearly there ...
 
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  • #10
BvU said:
Hoho! Not yet! I'll let you know when I'm happy :wink:

As long as you write
I'm not happy by a long shot ! And the last bit ##e^{\ln y} = \frac{1}{y} ## is (probably :rolleyes:?) a typo, so that does not count.

Oops a typo indeed. Let's go slowly

I meant that a solution for ##(2)## is given by

\begin{equation*}
f(y,t) = e^{\ln y} = y
\end{equation*}

Next step would be going to ##(1)## and solve for ##g(y,t)##, wouldn't it?
 
  • #11
No: any function of ##t## can be factored in in both terms of ##(2)## without affecting the validity of the equation.
 
  • #12
BvU said:
By the way, we physicists usually write ##e^{-\ln y} \ ## as ##\ \displaystyle{1\over y}\ ##
As do mathematicians...
 
  • #13
BvU said:
No: any function of ##t## can be factored in in both terms of ##(2)## without affecting the validity of the equation.

I better take more time to study and then reply. I do not want to exhaust your patience 😅
 

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