Solve the Partial differential equation ##U_{xy}=0##

  • #1
chwala
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I am going through these notes; i want to check that i am gettting it right...

Solve the pde;

##U_{xy}=0##
This is part of the notes;

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My own way of thought;

Given;

##U_{xy}=0##

then considering ##U_x## as on ode in the ##y## variable; we integrate both sides with respect to ##y## i.e

##\dfrac{du}{dx} \int \dfrac{1}{dy} dy=\int 0 dy##

this is the part i need insight...the original problem involves partial derivatives but in this case when we integrate with respect to ##y## we are integrating with respect to ##dy## and not ##∂y## ...correct?

##U_x= 0 + k##, where ##k## is a constant in terms of ##x## therefore,

##U_x= f(x)##, an arbitrary function of ##x##... which is an ode for ##u## in the ##x## variable. On integrating again with respect to ##x## we get,##U(x,y) = F(x) + k##, where ##k## is a constant in terms of ##y## therefore,

##U(x,y) = F(x) + H(y)##cheers!
 
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  • #2
I interpret you as follows.
[tex]\frac{\partial^2 U(x,y)}{\partial x \partial y}=0[/tex]
Integration by y with x=const. or by x with y=const.
[tex]\frac{\partial U}{\partial x }=f(x)[/tex]
[tex]\frac{\partial U}{\partial y }=g(y)[/tex]
Thus
[tex]dU=f(x)dx+g(y)dy[/tex]
[tex]U(x,y)=F(x)+G(y)[/tex]
 
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  • #3
anuttarasammyak said:
I interpret you as follows.
[tex]\frac{\partial^2 U(x,y)}{\partial x \partial y}=0[/tex]
Integration by y with x=const. or by x with y=const.
[tex]\frac{\partial U}{\partial x }=f(x)[/tex]
[tex]\frac{\partial U}{\partial y }=g(y)[/tex]
Thus
[tex]dU=f(x)dx+g(y)dy[/tex]
[tex]U(x,y)=F(x)+G(y)[/tex]
Is there another way bro? ...they call it method of characteristic ...need to read on this...
 
  • #4
chwala said:
Given;
##U_{xy}=0##

then considering ##U_x## as on ode in the ##y## variable; we integrate both sides with respect to ##y## i.e

##\dfrac{du}{dx} \int \dfrac{1}{dy} dy=\int 0 dy##
The above doesn't make any sense to me. Clearly the last integral would be 0 + a constant.
chwala said:
this is the part i need insight...the original problem involves partial derivatives but in this case when we integrate with respect to ##y## we are integrating with respect to ##dy## and not ##∂y## ...correct?
The expression ##dy## serves only to indicate the variable with respect to which integration is taking place. You are integrating with respect to y, not dy, and definitely not with respect to ∂y.
 
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