Apply Gauss's theorem when the metric is unknown

In summary: Y_2=(u^1-u^1)\frac{\partial}{\partial u^1}+(u^2-u^2)\frac{\partial}{\partial u^2}$. Now, we can apply the Gauss theorem separately to each of these two vector fields. For $Y_1$, we can use the same computation as before, as $Y_1=X$ outside of $F_1$ and $Y_1=0$ on $F_1$. For $Y_2$, we can use the fact that $Y_2=0$ on $F_1$ and therefore does not contribute to the integral over $
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Let $$f:U \to \mathbb{R}^3$$ be a surface, where $$U=\{(u^1,u^2)\in \mathbb{R}^2:|u^1|<3, |u^2|<3\}.$$ Consider the two closed square regions $$4F_1=\{(u^1,u^2)\in \mathbb{R}^2:|u^1|\leq1, |u^2|\leq1\}$$ and $$F_2=\{(u^1,u^2)\in \mathbb{R}^2:|u^1|\leq2, |u^2|\leq2\}.$$

While the first fundamental form $$g$$ is unknown in the inner region $$F_1$$, it is the Euclidean metric outside of $$F_1$$:$$g=(\mathrm{d}u^1)^2+(\mathrm{d}u^2)^2$$ at all $$u\in U-F_1$$
Also, it is known that the vector field $$X=u^1\frac{\partial}{\partial u^1}+u^2\frac{\partial}{\partial u^2}$$ satiesfies $$\mathrm{div}X=2$$ for ALL points of U.
Show that the total surface area of $$f(F_2)$$ is 16.Remark: Recall that the Gauss theorem states: Let $$M$$ be an oriented surface with a Riemannian metric. Let $$X$$ be a vector field on $$M$$. Then for each polygon on $$M$$ given by $$P:F \to M$$ it has $$\int_{P(F)}(\mathrm{div}X)\mathrm{d}M=\int_{\partial P(F)}l_{X}\mathrm{d}M$$,where $$l_{X}\mathrm{d}M=-X^2\sqrt|g|\mathrm{d}u^1+X^1\sqrt|g|\mathrm{d}u^2$$.

,Setting $$f_1:=-X^2\sqrt|g|$$ and $$f_2:=X^1\sqrt|g|$$ to get $$\int_{P(F)}(\mathrm{div}X)\mathrm{d}M=\iint_F}(\frac{\partial f_2}{\partial u^1}-\frac{\partial f_1}{\partial u^2})\mathrm{d}u^1\mathrm{d}u^2.$$

In this problem $|g|=1$ outside $F_1$ but it's unknown on $F_1$.

We need to compute $$\int_{f(F_2)}\mathrm{d}M=\frac{1}{2}\int_{f(F_2)}(\mathrm{div}X)\mathrm{d}M$$. By the convention of notations it has $X^i=u^i$ and thus $$\frac{1}{2}\int_{f(F_2)}(\mathrm{div}X)\mathrm{d}M=\frac{1}{2}\int_{-2}^{2}\int_{-2}^{2}(1-(-1))\mathrm{d}u^1\mathrm{d}u^2=16.$$

BUT my computation assumes $$g$$ is also the Euclidean metric on $$F_1$$, which may not be the case. How to modify my computation for it to be fully correct?
 
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Thank you for bringing up this interesting problem. As you correctly pointed out, your computation assumes that the metric $g$ is also the Euclidean metric on $F_1$. To modify your computation to be fully correct, we need to take into account the fact that the metric $g$ is unknown on $F_1$.

To do this, we can use the Gauss theorem as stated in the problem, but instead of using the vector field $X=u^1\frac{\partial}{\partial u^1}+u^2\frac{\partial}{\partial u^2}$, we can use a new vector field $Y=u^1\frac{\partial}{\partial u^1}+u^2\frac{\partial}{\partial u^2}$ that is defined as follows:

- On $F_1$, we define $Y$ to be the zero vector field, as the metric $g$ is unknown on $F_1$ and we cannot use the Gauss theorem in this region.

- Outside of $F_1$, we define $Y$ to be equal to $X$, i.e. $Y=u^1\frac{\partial}{\partial u^1}+u^2\frac{\partial}{\partial u^2}$.

With this new vector field $Y$, we can still use the Gauss theorem to compute the surface area of $f(F_2)$, but now we have to take into account the fact that $Y$ is not a constant vector field on $F_1$. This means that we have to modify the integral in the Gauss theorem to take into account the variation of $Y$ on $F_1$.

To do this, we can write $Y$ as $Y=u^1\frac{\partial}{\partial u^1}+u^2\frac{\partial}{\partial u^2}=u^1\frac{\partial}{\partial u^1}+u^2\frac{\partial}{\partial u^2}+(u^1-u^1)\frac{\partial}{\partial u^1}+(u^2-u^2)\frac{\partial}{\partial u^2}$. This allows us to write $Y$ as the sum of two vector fields $Y_1=u^1\frac{\partial}{\partial u^1}+u^
 

FAQ: Apply Gauss's theorem when the metric is unknown

What is Gauss's theorem?

Gauss's theorem, also known as the divergence theorem, is a fundamental theorem in vector calculus that relates a surface integral over a closed surface to a volume integral over the region bounded by that surface.

How does Gauss's theorem apply when the metric is unknown?

Gauss's theorem can still be applied when the metric is unknown by using an alternative form of the theorem that involves a scalar potential function. This allows for the calculation of the surface integral using only the boundary of the region, rather than the metric itself.

What are some real-world applications of Gauss's theorem when the metric is unknown?

Gauss's theorem has many applications in various fields, including fluid dynamics, electromagnetism, and thermodynamics. For example, it can be used to calculate the flow of a fluid through a given surface, or the electric flux through a closed surface containing a charge.

Are there any limitations to applying Gauss's theorem when the metric is unknown?

One limitation is that Gauss's theorem only applies to closed surfaces, so it cannot be used in situations where the surface is not closed. Additionally, the scalar potential function used in the alternative form of the theorem may not always exist or be easily determined in some cases.

How does Gauss's theorem relate to other fundamental theorems in mathematics?

Gauss's theorem is closely related to other fundamental theorems in mathematics, such as Green's theorem and Stokes' theorem. In fact, Green's theorem can be seen as a special case of Gauss's theorem when the surface is a plane, and Stokes' theorem can be derived from Gauss's theorem by letting the surface approach a point.

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