Can we find the interior of the given curve using Green's theorem?

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Discussion Overview

The discussion revolves around the application of Green's theorem to compute a line integral and explore the interior of a curve defined parametrically. Participants examine the implications of the theorem, the setup of integrals in different coordinate systems, and the conditions under which certain mathematical expressions are defined.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant computes the integral using Green's theorem and questions the implications of a zero result on finding the interior of the curve.
  • Another participant suggests setting up the integral in Cartesian coordinates and discusses the symmetry of the region.
  • There is a discussion on the conditions under which the expression for \(y\) derived from \(x\) is valid, particularly regarding the positivity of the square root.
  • Several participants explore the definition of \(x^{2/3}\) for negative \(x\) and the implications of different evaluation orders on the validity of power identities.
  • One participant proposes a more general integral that encompasses both positive and negative values of \(x\), while another questions the derivation of limits for \(x\).
  • Participants express confusion over the properties of exponentiation and the conditions under which certain mathematical identities hold.

Areas of Agreement / Disagreement

There is no consensus on several points, including the definition of powers for negative numbers, the validity of certain mathematical identities, and the best approach to setting up the integral. Participants express differing views on these topics, leading to ongoing debate.

Contextual Notes

Limitations include unresolved assumptions about the definitions of mathematical expressions, the conditions under which certain integrals are valid, and the implications of symmetry in the region of integration.

evinda
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Hello! (Wave)

Using Green's theorem, I want to compute the integral

$$\oint_C ydx+xdy$$

where $C$ has the parametric representation $r(t)=2 \cos^3 t i+ 2 \sin^3 t j, (0 \leq t \leq 2 \pi)$.

Using Green's theorem, we get that $\oint_C ydx+xdy=\iint_U (1-1)dxdy=0$.

I am wondering if we could find the interior $U$ of the curve $C$. I.e. if the result wouldn't be $0$, could we compute the double integral that we get? (Thinking)
 
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Hey evinda! (Smile)

To calculate the integral we can either try to set it up in polar or in cartesian coordinates.

To get cartesian coordinates we have in the first quadrant:
$$x=2\cos^3t \quad\Rightarrow\quad
t=\arccos \left((x/2)^{1/3}\right) \quad\Rightarrow\quad \\
y=2\sin^3 t = 2\sin^3\left(\arccos \left((x/2)^{1/3}\right)\right) = 2\left(\sqrt{1-(x/2)^{2/3}}\right)^3
= 2\left(1-(x/2)^{2/3}\right)^{3/2}
$$
Note that $U$ has horizontal and vertical reflection symmetry.
So:
$$
\iint_U f(x,y) dxdy = \int_0^2 \int_{-2\left(1-(x/2)^{2/3}\right)^{3/2}}^{2\left(1-(x/2)^{2/3}\right)^{3/2}} f(x,y)dydx + \text{almost same integral for negative x}
$$
If $f(x,y)=1$, Wolfram can come up with a closed form.
See here.
It's not a particularly easy integral to find by hand, but it seems doable.

And of course it changes if $f(x,y)$ is not a constant, in which case it can become easier or more complicated. (Thinking)
 
Using the fact that

$$\sin^2\left(\arccos \left(\left(\frac{x}{2}\right)^{\frac{1}{3}}\right)\right)+\cos^2\left(\arccos\left(\left(\frac{x}{2}\right)^{\frac{1}{3}}\right)\right)=1$$

we get that

$$\sin\left(\arccos\left(\frac{x}{2}\right)^{\frac{1}{3}}\right)=\pm \sqrt{1-\left(\frac{x}{2}\right)^{\frac{2}{3}}}$$

So it follows that $y=\pm 2 \left( 1-\left( \frac{x}{2}\right)^{\frac{2}{3}}\right)^{\frac{3}{2}}$.

Since $1-\left( \frac{x}{2}\right)^{\frac{2}{3}}$ is an expression under the square root, it must be positive, and so it follows that $x \leq 2$. How do we get that $x \geq 0$ ? (Thinking)
 
evinda said:
Since $1-\left( \frac{x}{2}\right)^{\frac{2}{3}}$ is an expression under the square root, it must be positive, and so it follows that $x \leq 2$. How do we get that $x \geq 0$ ? (Thinking)

It's just that $x^{2/3}$ is not defined for negative $x$. (Worried)

Then again, if we write it as $(x^2)^{1/3}$ it would be fine. (Thinking)
 
I like Serena said:
It's just that $x^{2/3}$ is not defined for negative $x$. (Worried)

Why isn't $x^{2/3}$ defined for negative $x$? (Thinking)
 
evinda said:
Why isn't $x^{2/3}$ defined for negative $x$? (Thinking)

Behold:
$$-1=(-1)^{\frac 23 \cdot \frac 32} = \left((-1)^{\frac 23}\right)^{\frac 32} = 1^{\frac 32} = 1$$
yes?
... but isn't $-1\ne 1$? (Sweating)

Can you spot the problem? (Wondering)
 
I like Serena said:
Behold:
$$-1=(-1)^{\frac 23 \cdot \frac 32} = \left((-1)^{\frac 23}\right)^{\frac 32} = 1^{\frac 32} = 1$$
yes?
... but isn't $-1\ne 1$? (Sweating)

Can you spot the problem? (Wondering)
We have that $x=x^{\frac{2}{3} \cdot \frac{3}{2}}=(x^{\frac{3}{2}})^{\frac{2}{3}}$.

Since $x^{\frac{3}{2}}=x \sqrt{x}$, $x$ has to be $\geq 0$, right?
 
evinda said:
We have that $x=x^{\frac{2}{3} \cdot \frac{3}{2}}=(x^{\frac{3}{2}})^{\frac{2}{3}}$.

Since $x^{\frac{3}{2}}=x \sqrt{x}$, $x$ has to be $\geq 0$, right?

If we would evaluate the expression in that order, then yes, $x$ has to be $\geq 0$.
But in the order I wrote it, that is not required, is it? (Wondering)
Either way, yes, we can see that the order in which we evaluate the powers makes a difference.

To be fair, we can define $x^{2/3}$ for negative $x$, so that $(-x)^{2/3}=x^{2/3}$.
It's just that if do, we can no longer use the power identity $a^{bc}=(a^b)^c$ as it breaks down.
It's one or the other.
So generally $x^\alpha$ is not defined for negative $x$ if $\alpha$ is a rational or real number that is not an integer. (Nerd)

Just for fun, let's see what W|A makes of it:
(-1)^(2/3) - Wolfram|Alpha Results
Hey, where did that come from? (Wondering)
 
I like Serena said:
To be fair, we can define $x^{2/3}$ for negative $x$, so that $(-x)^{2/3}=x^{2/3}$.
It's just that if do, we can no longer use the power identity $a^{bc}=(a^b)^c$ as it breaks down.
It's one or the other.

I am confused now. Doesn't this property always hold? (Thinking)
 
  • #10
evinda said:
I am confused now. Doesn't this property always hold? (Thinking)

Indeed, that power identity does not always hold.
See the section Failure of power and logarithm identities in the Exponentation wiki article to see how it breaks down for complex numbers. (Worried)
 
  • #11
I like Serena said:
$$
\iint_U f(x,y) dxdy = \int_0^2 \int_{-2\left(1-(x/2)^{2/3}\right)^{3/2}}^{2\left(1-(x/2)^{2/3}\right)^{3/2}} f(x,y)dydx + \text{almost same integral for negative x}
$$

Here, how did you find this one: $\int_0^2 \int_{-2\left(1-(x/2)^{2/3}\right)^{3/2}}^{2\left(1-(x/2)^{2/3}\right)^{3/2}} f(x,y)dydx + \text{almost same integral for negative x}$ ? (Worried)

I mean, isn't there a formula that holds for all $x$ ? Instead of considering some integral for negative $x$ ?
 
  • #12
evinda said:
Here, how did you find this one: $\int_0^2 \int_{-2\left(1-(x/2)^{2/3}\right)^{3/2}}^{2\left(1-(x/2)^{2/3}\right)^{3/2}} f(x,y)dydx + \text{almost same integral for negative x}$ ? (Worried)

I mean, isn't there a formula that holds for all $x$ ? Instead of considering some integral for negative $x$ ?

Yes, I believe we can make it:
$$\int_{-2}^2 \int_{-2\left(1-((x/2)^2)^{1/3}\right)^{3/2}}^{2\left(1-((x/2)^2)^{1/3}\right)^{3/2}} f(x,y)dydx$$
I just tried to avoid that profusion of parentheses. (Wasntme)
 
  • #13
I like Serena said:
Yes, I believe we can make it:
$$\int_{-2}^2 \int_{-2\left(1-((x/2)^2)^{1/3}\right)^{3/2}}^{2\left(1-((x/2)^2)^{1/3}\right)^{3/2}} f(x,y)dydx$$
I just tried to avoid that profusion of parentheses. (Wasntme)

From which relation do we get that $x \geq -2$? (Thinking)
 
  • #14
evinda said:
From which relation do we get that $x \geq -2$?

We have $x=2\cos^3 t$, meaning that $-2 \le x \le 2$. (Thinking)
 
  • #15
I like Serena said:
We have $x=2\cos^3 t$, meaning that $-2 \le x \le 2$. (Thinking)

I see... Thanks a lot! (Smirk)
 

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