Why can one do this "trick" in the First Order Linear D.E. method?

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In summary, the "trick" in solving First Order Linear Differential Equations (D.E.) involves using an integrating factor to simplify the equation into an easily solvable form. This technique leverages the linearity of the equation, allowing one to multiply through by a specific function that transforms the left-hand side into the derivative of a product, facilitating straightforward integration and solution derivation.
  • #1
Ebby
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Homework Statement
Explain the First Order Linear D.E. method
Relevant Equations
Can you explain the step shown below?
If we have a first order d.e. like: $$\frac {dy} {dx} - \frac y x = 1$$
I would use two subs, namely: ##y = uv## and ##\frac {dy} {dx} = u \frac {dv} {dx} + v \frac {du} {dx}##

So I get: ##\frac {dy} {dx} = u \frac {dv} {dx} + v \frac {du} {dx} - \frac {uv} {x} = 1##

I then factor like this: ##\frac {dy} {dx} = u \frac {dv} {dx} + v (\frac {du} {dx} - \frac {u} {x}) = 1##

I am then told that I can make ##\frac {du} {dx} - \frac {u} {x} = 0##. *Why* can I do this?
 
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  • #2
Ebby said:
Homework Statement: Explain the First Order Linear D.E. method
Relevant Equations: Can you explain the step shown below?

If we have a first order d.e. like: $$\frac {dy} {dx} - \frac y x = 1$$
I would use two subs, namely: ##y = uv## and ##\frac {dy} {dx} = u \frac {dv} {dx} + v \frac {du} {dx}##

So I get: ##\frac {dy} {dx} = u \frac {dv} {dx} + v \frac {du} {dx} - \frac {uv} {x} = 1##

I then factor like this: ##\frac {dy} {dx} = u \frac {dv} {dx} + v (\frac {du} {dx} - \frac {u} {x}) = 1##

I am then told that I can make ##\frac {du} {dx} - \frac {u} {x} = 0##. *Why* can I do this?
Are you sure the trick isn't ## y = u x ##?

$$ \frac{dy}{dx} = \frac{du}{dx}x + u $$

Then sub for ## \frac{dy}{dx}##

$$\frac{du}{dx}x + u - u = 1 $$

$$ \implies \frac{du}{dx} = \frac{1}{x} $$

?
 
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  • #3
Just solve ##u’(x) = u/x##. This is a simple homogeneous ODE with the general solution ##u(x) = Ax## for any constant ##A##.
 
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  • #4
If the question is why you are allowed to pick a ##u## such that the ODE is satisfied: The substitution is valid for any ##u##.* The trick is to pick a ##u## such that the resulting ODE for ##v## takes a simpler form that allows you to solve it.

* Not any function of course. Suitable requirements on differentiability and not introducing additional zeros apply.
 
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  • #5
Ebby said:
Homework Statement: Explain the First Order Linear D.E. method
Relevant Equations: Can you explain the step shown below?

If we have a first order d.e. like: $$\frac {dy} {dx} - \frac y x = 1$$
I would use two subs, namely: ##y = uv## and ##\frac {dy} {dx} = u \frac {dv} {dx} + v \frac {du} {dx}##

So I get: ##\frac {dy} {dx} = u \frac {dv} {dx} + v \frac {du} {dx} - \frac {uv} {x} = 1##

I then factor like this: ##\frac {dy} {dx} = u \frac {dv} {dx} + v (\frac {du} {dx} - \frac {u} {x}) = 1##

I am then told that I can make ##\frac {du} {dx} - \frac {u} {x} = 0##. *Why* can I do this?
I doubt it too, just like @erobz . If you could do that, I your second expression in the equality would be 0, and in your chain of equalities, you would end up with ##\frac {dy}{dx}=1##, from which it follows that ##f(x)=x## is a solution, which it isn't , for your initial equation.
 
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  • #6
Ebby said:
Homework Statement: Explain the First Order Linear D.E. method
Relevant Equations: Can you explain the step shown below?

*Why* can I do this?
You can choose any ##u## OR any ##v## that makes the solution process easier. If you pick a certain ##u##, you got to adjust the ##v## accordingly so that ##v=\frac{y}{u}## and similar if you chose a certain ##v##.

Beware that the "OR" is exclusive, that is you are not free to choose both of ##u ,v## because as i said before if you choose one the other becomes chosen already as y/"what you chose at first step".

Try choosing as ##v=c## that is a constant and see what happens too.
 
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  • #7
he has a typo in his second long equality

It should be $$\frac{dy}{dx}-\frac{y}{x}=...$$
 
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  • #8
WWGD said:
I doubt it too, just like @erobz . If you could do that, I your second expression in the equality would be 0, and in your chain of equalities, you would end up with ##\frac {dy}{dx}=1##, from which it follows that ##f(x)=x## is a solution, which it isn't , for your initial equation.
As @Delta2 says, that’s just a typo in the OP. The original statement is
Ebby said:
##\frac {dy} {dx} = u \frac {dv} {dx} + v \frac {du} {dx}##
and the typo comes right after:
Ebby said:
So I get: ##\frac {dy} {dx} = u \frac {dv} {dx} + v \frac {du} {dx} - \frac {uv} {x} = 1##
where OP has forgotten to add ##-y/x## to the RHS.

The actual ODE leads to
$$
\frac{dv}{dx} = \frac{1}{Ax}
$$
where ##y(x) = Ax \,v(x)##.
 
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  • #9
I don't know what this whole idea about making substitutions is but I'm sure it amounts to the following:

The idea is to make the left side into a product rule via an integrating factor

If you have the equation

##\frac{dy}{dx} +p(x) y = g(x)##

If you multiply through by an "integrating factor" ## \mu \left(x\right) = e^{\int p(x)\,dx}## you will make the left hand side into a product rule.

In your case

##\frac{dy}{dx} + \left( - \frac{1}{x} \right) y = 1##

multiply through by ##\mu \left(x \right) = e^{\int -\frac{1}{x} \,dx} = \frac{1}{x}## which leads to

##\frac{1}{x} \frac{dy}{dx} - \frac{y}{x^2} = \frac{1}{x}##

Recognize the left as a product rule

##\frac{d}{dx} \left( \frac{y}{x}\right) = \frac{1}{x}##

Integrate both sides accounting for a "constant of integration" then isolate ##y## from ##x##

Plug it into the original differential equation and it works

This strategy is pretty standard, more on the "integrating factor" https://tutorial.math.lamar.edu/classes/de/linear.aspx
 
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  • #10
PhDeezNutz said:
I don't know what this whole idea about making substitutions is but I'm sure it amounts to the following:

The idea is to make the left side into a product rule via an integrating factor

If you have the equation

##\frac{dy}{dx} +p(x) y = g(x)##

If you multiply through by an "integrating factor" ## \mu \left(x\right) = e^{\int p(x)\,dx}## you will make the left hand side into a product rule.

In your case

##\frac{dy}{dx} + \left( - \frac{1}{x} \right) y = 1##

multiply through by ##\mu \left(x \right) = e^{\int -\frac{1}{x} \,dx} = \frac{1}{x}## which leads to

##\frac{1}{x} \frac{dy}{dx} - \frac{y}{x^2} = \frac{1}{x}##

Recognize the left as a product rule

##\frac{d}{dx} \left( \frac{y}{x}\right) = \frac{1}{x}##

Integrate both sides accounting for a "constant of integration" then isolate ##y## from ##x##

Plug it into the original differential equation and it works

This strategy is pretty standard, more on the "integrating factor" https://tutorial.math.lamar.edu/classes/de/linear.aspx
This is similar to the idea for finding weak solutions to DEs.
 
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  • #11
WWGD said:
This is similar to the idea for finding weak solutions to DEs.
Didn't know that but now with that knowledge I have a direction to look in with insight you have given me!
 
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  • #13
Ebby said:
I'm a bit confused because apparently I've made a typo but I simply used an example from this site about DEs (it's Example 1): https://www.mathsisfun.com/calculus/differential-equations-first-order-linear.html

Where exactly did I go wrong?
Ehm, except the typo you didn't do anything else wrong, you are right that you can choose a ##u## such that
$$\frac{du}{dx}-\frac{u}{x}=0$$, or any other condition that helps solve the ODE.
 
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  • #14
OK, I see the typo now. Phew. But let me ask the really dumb question:

Given that: $$u \frac {dv} {dx} + v(\frac {du} {dx} - \frac u x) = 1$$

Why can we say that, algebraically: $$\frac {du} {dx} - \frac u x = 0$$

? I know, I'm really stupid...
 
  • #15
You got to try to read -while paying some attention -of all the previous posts here

But anyway I am gonna say it again.

You CAN CHOOSE a ##u## such that ##\frac{du}{dx}-\frac{u}{x}=0##. You are free to choose any ##u## you like. You are also free to choose any ##v## you like. But not both.
 
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  • #16
Ebby said:
OK, I see the typo now. Phew. But let me ask the really dumb question:

Given that: $$u \frac {dv} {dx} + v(\frac {du} {dx} - \frac u x) = 1$$

Why can we say that, algebraically: $$\frac {du} {dx} - \frac u x = 0$$

? I know, I'm really stupid...
Post #4, extra emphasis:
Orodruin said:
If the question is why you are allowed to pick a ##u## such that the ODE is satisfied: The substitution is valid for any ##u##.* The trick is to pick a ##u## such that the resulting ODE for ##v## takes a simpler form that allows you to solve it.

* Not any function of course. Suitable requirements on differentiability and not introducing additional zeros apply.
 
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  • #17
Ok I kinda am within your mind and now you ask
"Why I am free to choose any u i like???, u, v are supposed to be specific functions"

##u , v## are just functions that satisfy ##y=uv## (and y satisfies that given ODE).

But ##u,v## are not so specific.
Lets say for example that ##y=x^4+x^2## (i dont think that this y satisfies the given ODE but it doesnt matter you ll see my point as you go on reading here)

You can write ##y=x^2(x^2+1)## or ##y=x^3(x+\frac{1}{x})##

So you can choose as ##u=x^2, v=x^2+1## or ##u=x^3, v=x+\frac{1}{x}##

I think now you should be able to understand why u,v are not so specific.
 
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  • #18
I mean, you could choose ##u = e^{x + 4i}- \ln(x^x)##, but that would not make the differential equation for ##v## any simpler. The trick is to pick a ##u## that makes the ODE for ##v## simpler. In this case, such a ##u## satisfies that particular ODE because that means a term disappears.
 
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  • #19
Even if one wants to choose as ##u## as given at post #18, you can choose as ##v=\frac{x^4+x^2}{e^{x+4i}-\ln{x^x}}## and again you will have that ##y=uv## holds.
 
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  • #20
Thank you. I now understand.

I think if someone had said, "Think that you are choosing to make ## \frac {du} {dx} = \frac u x ## so that the ## v ## term disappears, rather than thinking ## \frac {du} {dx} - \frac u x = 0 ##," it would have been clearer to me. Anyway, thank you all. This has been helpful in a more far reaching sense.
 
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FAQ: Why can one do this "trick" in the First Order Linear D.E. method?

What is the First Order Linear Differential Equation method?

The First Order Linear Differential Equation method is a technique used to solve differential equations of the form \( \frac{dy}{dx} + P(x)y = Q(x) \). This method involves finding an integrating factor, which simplifies the equation into a form that can be easily integrated.

Why do we use an integrating factor in solving First Order Linear D.E.s?

An integrating factor is used to transform the differential equation into an exact equation. By multiplying the entire differential equation by this integrating factor, the left-hand side becomes the derivative of a product of functions, which can then be integrated directly to find the solution.

How is the integrating factor determined?

The integrating factor is determined by the function \( P(x) \) in the differential equation. It is given by \( \mu(x) = e^{\int P(x) \, dx} \). This factor, when multiplied by the original differential equation, allows the left-hand side to be written as a single derivative.

Why does the integrating factor work to simplify the equation?

The integrating factor works because it converts the non-exact differential equation into an exact one. By design, it ensures that the left-hand side of the equation becomes the derivative of a product of two functions, making the equation easier to integrate and solve.

Can the First Order Linear D.E. method be applied to non-linear differential equations?

No, the First Order Linear D.E. method is specifically designed for linear differential equations of the first order. Non-linear differential equations require different techniques and methods for their solutions, as the properties and behaviors of non-linear equations are fundamentally different from linear ones.

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