Line Integral of circle in counterclockwise direction

  • #1
songoku
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Homework Statement
Please see below
Relevant Equations
Line Integral
Parametric
1701323428594.png


My attempt:
Let ##x=a \cos \theta## and ##y=a \sin \theta##

$$\int_{L} xy^2 dx-x^2ydy$$
$$=\int_{0}^{2\pi} \left( (a\cos \theta)(a\sin \theta)^2 (-a\sin \theta)-(a\cos \theta)^2 (a \sin \theta)(a\cos \theta)\right) d\theta$$
$$=-a^4 \int_{0}^{2\pi}\left( \sin^3 \theta \cos \theta+\cos^3 \theta \sin \theta \right) d\theta$$

I get zero as the result of the integration. Is it possible? Thanks
 
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  • #2
Yes, the integral is zero by symmetry.
 
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  • #3
Orodruin said:
Yes, the integral is zero by symmetry.
To qualify this:

Take the first term and consider the integral along the lower half-circle. You obtain ##y^2 = a^2 - x^2## and can parametrize it by ##-a < x < a##. The integral along the lower half-circle is therefore
$$
\int_{-a}^a y^2 x \, dx = \int_{-a}^a (a^2 - x^2) x \, dx
$$
which is an integral of an odd function over an even interval and therefore zero. A similar argument applies to the upper half-circle and for the integral of the other term.

Alternatively, you can use Green's formula and conclude that
$$
\oint_\Gamma \left(y^2 x \, dx - x^2 y \, dy\right)
= \int_{S} \left(-\frac{\partial(x^2 y)}{\partial x} - \frac{\partial(y^2 x)}{\partial y}\right) dx\, dy
= - 4 \int_{S} xy \, dx\, dy,
$$
where ##S## is the disc enclosed by the circle. This integral is obviously zero since the integrand is odd in both ##x## and ##y## whereas ##S## is symmetric with respect to ##x \to -x## as well as ##y \to -y##.
 
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  • #4
Thank you very much for the help and explanation Orodruin
 
  • #5
FYI, there is a very large class of functions that will give zero integrals on closed curves. They are related to potentials and to analytic functions with no enclosed singularities.
 
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  • #6
FactChecker said:
FYI, there is a very large class of functions that will give zero integrals on closed curves. They are related to potentials and to analytic functions with no enclosed singularities.
Should be pointed out that this is not the case here though. The zero really comes from symmetry. This may be seen from the fact that the integrand of the area integral in Green’s formula above is not zero so there will exist areas such that the integral around them are non-zero.

(Yes, I tried that first before arguing symmetry 😉)
 
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FAQ: Line Integral of circle in counterclockwise direction

What is a line integral in the context of a circle?

A line integral in the context of a circle is a type of integral where a function is evaluated along a curve, specifically the circumference of the circle. It often involves integrating a scalar or vector field along the path defined by the circle.

How do you parametrize a circle for a line integral?

To parametrize a circle for a line integral, you typically use the parametric equations x = r*cos(t) and y = r*sin(t), where r is the radius of the circle and t is the parameter that ranges from 0 to 2π for a complete traversal of the circle.

What does it mean to integrate in the counterclockwise direction?

Integrating in the counterclockwise direction means that the parameter t increases from 0 to 2π, following the positive orientation around the circle. This is the standard direction for positive orientation in mathematics.

How do you set up a line integral around a circle in a vector field?

To set up a line integral around a circle in a vector field, you need to parametrize the circle and then substitute these parametric equations into the vector field. The line integral is then computed as the integral of the dot product of the vector field and the differential position vector along the path of the circle.

What is the significance of the line integral around a closed curve like a circle?

The line integral around a closed curve like a circle is significant in many areas of physics and engineering, such as calculating circulation and flux in fluid dynamics and electromagnetism. It is also related to important theorems like Green's Theorem, which relates the line integral around a closed curve to a double integral over the region enclosed by the curve.

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