When the integral of total derivative[tex] \oint d U = 0 [/tex]?,

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In summary, the conversation discusses the integral of total derivative and the conditions for it to be equal to zero. Alex asks about the region of integration and the definition of y. The discussion leads to a theorem stating that the integral equals zero if the differential form is exact. The conversation also touches on the topic of contour integration and the definition of y on a circle. Ultimately, it is determined that the integral \oint e^{|\theta|} d\theta is not zero due to the singularity at (0,0) and the form not being globally defined.
  • #1
alejandrito29
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when the integral of total derivative[tex] \oint d U = 0 [/tex]?,

when the integral of total derivative
[tex] \oint d U = 0 [/tex]?, and ¿why is zero?

and,

when

[tex] \oint d U \neq 0 [/tex] ??
 
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  • #2


Alex: are you integrating the identity? And, what is the region over which you are
integrating?
 
  • #3


The closed line integral dU = 0 if dU is an exact differential. U is then a state function and by definition if you end up where you started you get zero.

Think of a closed line integral of gravitational or electrostatic force.
 
  • #4


An example , a classical one, I think, of a form that is not exact is that of w=dz/z

defined on the circle |z|=1, embedded in R-{(0,0)}, or C-{(0,0)} .
 
  • #5


Bacle said:
Alex: are you integrating the identity? And, what is the region over which you are
integrating?

my problem is

[tex] \oint d( \frac{dA}{dy} exp(A) ) [/tex]

where [tex]A=|y|[/tex]
but, y is a angular coordinate...betwen [tex] )-\infty, \infty([/tex]
but my problem is that
[tex] \frac{d|y|}{dy} = -1 , y \in )-\pi,0(, )\pi,2\pi(, etc[/tex]
[tex] \frac{d|y|}{dy} = 1 , y \in )0,\pi(, )2\pi,3\pi(, etc[/tex]
[tex] \frac{d|y|}{dy} = undefinided , y =-\pi,0,\pi...k \cdot \pi[/tex]
........................
but, if i integrate

[tex] \oint exp(|y|) [/tex] ¿why is it Non zero, if i too started and end in the same point (0 and 2pi por example)
 
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  • #6


Alex:
By a theorem; I think Stokes or one of its corollaries, your last integral equals zero iff , f (exp|y| , in our case) as a differential form, is exact, or, equivalently, if there is an F
in the region of definition, with dF= exp|y|.

I'm sorry, I still don't fully understand why y is positive in some regions, and negative in others. Do you have an explicit formula for it?

Still, if you know that your y is defined as you said, the only reason I can see for why
it is not zero, is that , it does not have a global antiderivative.
 
  • #7


question :

can i to say [tex] d \theta = \frac{1}{x^2+y^2} (-y dx +x dy ) [/tex]
since i am to integrate on a circle, and , since

[tex] x = 1 \cdot \cos (\theta) ; y = 1 \cdot \sin (\theta) [/tex]

and then

[tex] \oint e^{|\theta|} d \theta = \oint e^{| \sin^{-1} y|} \frac{1}{x^2+y^2} (-y dx +x dy ) \neq 0 [/tex] , since is not globally defined in [tex] x, y = 0,0 [/tex] ?
 
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  • #8


The standard way (the one I know : ) ) of doing line integrals/ contour integration is
by parametrizing the contour:

x=cosθ , so that dx=cosθdθ

y=sinθ , so that dy=sinθdθ

And then integrate from 0 to 2∏ ; since the singularity happens at (0,0), which is
not in the contour, you don't need to worry about this. Still, another way of testing
whether:

dθ:= (xdy -ydy)/(x2+y2)

is exact, is by integrating around a close contour. If the form is exact, it would then
integrate to 0, by an extension of the fundamental theorem of calculus.
 
  • #9


firts , sorry by many questions,

in my case, i need to integrate on te circle

but in a text says:

[tex](xdy -ydy)/(x^ 2+y^ 2)[/tex] it is not exact, since its integral along the unit circle is not 0... [tex] \int ^\pi_{-\pi} d\theta = 2 \pi[/tex]...
this is a argument for says that [tex] \oint e^{|\theta|} d\theta [/tex] is not zero??
 

FAQ: When the integral of total derivative[tex] \oint d U = 0 [/tex]?,

What is the meaning of the integral of total derivative [tex]\oint d U = 0[/tex]?

The integral of total derivative [tex]\oint d U = 0[/tex] is a mathematical expression that represents the conservation of energy in a system. It means that the total change in energy within a closed system, represented by the integral, is equal to zero. This indicates that energy is neither created nor destroyed, but rather conserved within the system.

How is the integral of total derivative [tex]\oint d U = 0[/tex] related to the laws of thermodynamics?

The integral of total derivative [tex]\oint d U = 0[/tex] is closely related to the first law of thermodynamics, which states that energy cannot be created or destroyed, only transferred or converted from one form to another. The integral represents the total change in energy within a system, and the fact that it equals zero indicates that energy is conserved according to the first law.

Can the integral of total derivative [tex]\oint d U = 0[/tex] be used to solve problems in physics and engineering?

Yes, the integral of total derivative [tex]\oint d U = 0[/tex] is a useful mathematical tool in solving problems related to energy conservation. It is commonly used in physics and engineering to analyze and understand the behavior of various systems, such as thermodynamic systems and control systems.

How is the integral of total derivative [tex]\oint d U = 0[/tex] calculated?

The integral of total derivative [tex]\oint d U = 0[/tex] is calculated using the principles of calculus. It involves taking the derivative of a function and then integrating it over a given range. The result is a numerical value that represents the total change in energy within the system.

What are the limitations of the integral of total derivative [tex]\oint d U = 0[/tex] in real-world applications?

While the integral of total derivative [tex]\oint d U = 0[/tex] is a valuable tool in understanding energy conservation, it has its limitations in real-world applications. It assumes that the system is closed and does not take into account external factors, such as energy loss or gain through heat transfer or work done by external forces. Additionally, it may not accurately represent complex systems with multiple energy sources and exchanges.

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