Solving the General Bernoulli / Riccati Equation

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In summary, the conversation discusses an equation of the form y'(t) + Ay(t) + By(t)^m + c = 0 and its different forms depending on the values of c and m. The question is raised about solving the general case of the equation and whether it can be converted to a Riccati or Bernoulli form. The response suggests setting new variables and separating the variables to solve the equation.
  • #1
crevoise
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Hello,

I have an equation of the following form: y'(t) + Ay(t) + By(t)^m + c = 0

1/ With c=0, the equation is of the Bernoulli form, and might be integrated.
2/ With m = 2, it is a Riccati equation, which might be turn back to a Bernoulli one and then integrated

3/ My question is about the general case, with c#0 and m a real (not only a natural). Does it exist some way to solve this general equation? Maybe there is a method to turn it back to Riccati or Benoulli shape?

Thanks a lot for your help

/crevoise
 
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  • #2
crevoise said:
Hello,

I have an equation of the following form: y'(t) + Ay(t) + By(t)^m + c = 0

1/ With c=0, the equation is of the Bernoulli form, and might be integrated.
2/ With m = 2, it is a Riccati equation, which might be turn back to a Bernoulli one and then integrated

3/ My question is about the general case, with c#0 and m a real (not only a natural). Does it exist some way to solve this general equation? Maybe there is a method to turn it back to Riccati or Benoulli shape?

Thanks a lot for your help

/crevoise

Let write the DE as...

$\displaystyle \frac{y^{\ '}+c}{y^{m}} + \frac{a}{y^{m-1}}=-b$ (1)

First we set...

$\displaystyle u=y+c\ x \implies u^{\ '}= y^{\ '} + c\ ,\ y^{m}= (u-c\ x)^{m} $ (2)

... so that (1) becomes...

$\displaystyle \frac{u^{\ '}} {(u-c\ x)^{m}} + \frac{a} {(u-c\ x)^{m-1}}= -b$ (3)

Now we set...

$\displaystyle v=\frac{1}{(u-cx)^{m-1}} \implies v^{\ '}= \frac{1-m}{(u-c\ x)^{m}}\ u^{\ '}$ (4)

... and if $m \ne 1$ the (3) becomes...

$\displaystyle \frac{v^{\ '}}{1-m} + a\ v = -b$ (5)

... which is linear...

Kind regards

$\chi$ $\sigma$
 
  • #3
chisigma said:
Let write the DE as...

$\displaystyle \frac{y^{\ '}+c}{y^{m}} + \frac{a}{y^{m-1}}=-b$ (1)

First we set...

$\displaystyle u=y+c\ x \implies u^{\ '}= y^{\ '} + c\ ,\ y^{m}= (u-c\ x)^{m} $ (2)

... so that (1) becomes...

$\displaystyle \frac{u^{\ '}} {(u-c\ x)^{m}} + \frac{a} {(u-c\ x)^{m-1}}= -b$ (3)

Now we set...

$\displaystyle v=\frac{1}{(u-cx)^{m-1}} \implies v^{\ '}= \frac{1-m}{(u-c\ x)^{m}}\ u^{\ '}$ (4)

... and if $m \ne 1$ the (3) becomes...

$\displaystyle \frac{v^{\ '}}{1-m} + a\ v = -b$ (5)

... which is linear...

Kind regards

$\chi$ $\sigma$

Hello,

Thanks a lot for your answer.
I think yet there is a small mistake on it, on the second change:

$\displaystyle v=\frac{1}{(u-cx)^{m-1}} \implies v^{\ '}= \frac{1-m}{(u-c\ x)^{m}}\ u^{\ '}$ (4)

I think it implies

$\displaystyle v^{\ '}= \frac{1-m}{(u-c\ x)^{m}}(\ u^{\ '}-c)$

isn't it?
 
  • #4
chisigma said:
Let write the DE as...

$\displaystyle \frac{y^{\ '}+c}{y^{m}} + \frac{a}{y^{m-1}}=-b$ (1)

First we set...

$\displaystyle u=y+c\ x \implies u^{\ '}= y^{\ '} + c\ ,\ y^{m}= (u-c\ x)^{m} $ (2)

... so that (1) becomes...

$\displaystyle \frac{u^{\ '}} {(u-c\ x)^{m}} + \frac{a} {(u-c\ x)^{m-1}}= -b$ (3)

Now we set...

$\displaystyle v=\frac{1}{(u-cx)^{m-1}} \implies v^{\ '}= \frac{1-m}{(u-c\ x)^{m}}\ u^{\ '}$ (4)

... and if $m \ne 1$ the (3) becomes...

$\displaystyle \frac{v^{\ '}}{1-m} + a\ v = -b$ (5)

... which is linear...

Kind regards

$\chi$ $\sigma$

You might want to check step (4).
 
  • #5
To the OP - Are A, B and C constant.
 
  • #6
Yes, A, B and C are constant for the moment.
 
  • #7
Then your ODE is separable. A much different animal if $A, B$ and $C$ are functions of $x$.
 
  • #8
chisigma said:
Let write the DE as...

$\displaystyle \frac{y^{\ '}+c}{y^{m}} + \frac{a}{y^{m-1}}=-b$ (1)

First we set...

$\displaystyle u=y+c\ x \implies u^{\ '}= y^{\ '} + c\ ,\ y^{m}= (u-c\ x)^{m} $ (2)

... so that (1) becomes...

$\displaystyle \frac{u^{\ '}} {(u-c\ x)^{m}} + \frac{a} {(u-c\ x)^{m-1}}= -b$ (3)

Proceeding in correct way from (3) now we set...

$\displaystyle v=\frac{1}{(u-cx)^{m-1}} \implies v^{\ '}= \frac{1-m}{(u-c\ x)^{m}}\ (u^{\ '}-c)$ (4)

... so that if $m \ne 1$ the (3) becomes in some steps...

$\displaystyle v^{\ '}= (m-1)\ (a\ v+ c\ v^{\frac{m}{m-1}}+ b)$ (5)

... where the variables are separated...

Kind regards

$\chi$ $\sigma$
 

Related to Solving the General Bernoulli / Riccati Equation

What is the Bernoulli equation?

The Bernoulli equation is a mathematical equation that relates pressure, density, and velocity of a fluid moving along a streamline. It is commonly used in fluid dynamics to analyze the flow of fluids in pipes and other systems.

What is the Riccati equation?

The Riccati equation is a type of differential equation that involves a quadratic term. It is often used in control theory to model systems that have feedback loops, such as in economics and engineering.

What is the relationship between the Bernoulli and Riccati equations?

The Bernoulli and Riccati equations are closely related as they both involve differential equations and are used to analyze fluid and control systems, respectively. In fact, the Bernoulli equation can be solved using the Riccati equation under certain conditions.

What are the applications of the Bernoulli and Riccati equations?

The Bernoulli equation is commonly used in fluid mechanics to analyze the flow of fluids in pipes and other systems. The Riccati equation has many applications in control theory and is used to model systems with feedback, such as in economics and engineering.

What are the limitations of the Bernoulli and Riccati equations?

The Bernoulli and Riccati equations have limitations in their applicability. The Bernoulli equation assumes that the fluid is incompressible, inviscid, and irrotational, which may not always be the case. The Riccati equation is limited to systems with feedback loops and may not accurately model more complex systems.

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