Homogeneous and particular solution

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The discussion revolves around solving the ordinary differential equation (ODE) Vz'' + (1/r)Vz' = k, where Vz represents velocity in the z direction and r is the independent variable. Participants clarify that Vz is the function to be solved for, and one contributor suggests using a substitution to simplify the equation. By multiplying the equation by r² and transforming it into a linear equation with constant coefficients, the solution is derived as Vz(r) = (k/4)r² + C1ln(r) + C2 after integrating twice. The conversation highlights the importance of correctly interpreting the variables and the steps involved in obtaining the general and particular solutions. Overall, the thread emphasizes the methodical approach to solving ODEs.
gomez
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hi,

I have this ODE and I need to obtain the general and the particular solution, this is the ODE

Vz''+1/r*Vz'= k

where k is a constant

thanks
 
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dextercioby said:
Who's "V"...?

Daniel.
I think it is a "she"..
 
Vz is just the velocity in the z direction, It's nothing more than my variable. Vz changed with respect to r.

Vz(r)''+1/r*Vz(r)' = k
 
Make the substitution

\frac{dv_{z}}{dr}=u(r)

Daniel.
 
I THINK (it surely isn't clear) that the OP mean that Vz is the function to be solved for.

Assuming also that r is the independent variable, we can multiply the entire equation by r2 to get the "Euler-type" (or "equipotential") equation r2Vz"+ rVz'= kr2. If we let x= ln r, (so that r= ex) we can rewrite that as a linear equation with constant coefficients. Specifically, (I'm writing "y" in place of "Vz" just because it is easier) dy/dr= dy/dx dx/dr= (1/r)(dy/dx) and d2y/dr2= d/dr((1/r)dy/dx)= (-1/r2(dy/dx)+ (1/r2)d2y/dx2.
The equation becomes d2y/dx2= ke2x. Integrating once, dy/dt= (k/2)e2x+ C1. Integrating a second time, y= (k/4)e2x+ C1x+ C2. ex= r so e2x= r2. In terms of r, y(r)= Vz(r)= (k/4)r2+ C1ln r+ C2.
 
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dextercioby said:
A what...?A "she"...?:confused:

Daniel.
Perhaps I was wrong then..
 

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