MyOpenMath/Solutions/Gauss law (TF)

These questions are inspired by MyOpenMath/Solutions/Gauss law (TF)/Proof

$$dA_1=dA_3\;?$$
This is NOT generally true. By the definition of solid angle, the projection of $$d\vec S$$ along the $$\hat r$$ does obey a conservation law. The surface area element is $$d\vec S = \hat n dA$$, and the projection of this surface along the radial $$\hat r$$ can be used to define the solid angle of a flux cone:


 * $$d\Omega =\frac {d\vec S_1\cdot \hat r}{r_1^2}=\frac {d\vec S_3\cdot \hat r}{r_3^2}

=\frac{\hat n_1\cdot\hat r dA_1}=\frac{\hat n_3\cdot\hat r dA_3}$$

Since $$\hat n_j\cdot\hat r=\cos\theta_j$$, we have:


 * $$\frac{dA_1}{dA_3}=\left(\frac{r_1}{r_3}\right)^2\left(\frac{\cos\theta_3}{\cos\theta_1}\right)$$

From the figure, $$r_3>r_1$$. But there is no hint as to the angle between the unit normal $$\hat n$$ and the radial unit vector $$\hat r$$, except that since the $$\vec r$$ exits the surface at both points, we know that:


 * $$\cos\theta_1 > 0 \text{ AND } \cos\theta_3 > 0 $$

While for some orientations of the surface areas at 1 and 3, the statement, $$dA_1=dA_3$$, could be true, the statement is not generally true. -

$$\vec {E_1}\cdot d \vec{S_1}=\vec{E_3}\cdot d \vec{S_3}\;?$$
This is generally true. Since the electric field falls as $$1/r^2$$ and points in the $$\hat r$$ direction, each term is directly proportional a solid angle. Moreover, since the flux cone exits at both points, the angle between the outward unit normal and the electric field is less than 90&deg;. It must be emphasized that this is true because there is only one point charge is present. -

$$\vec {E_1}\cdot d \vec{S_1}+\vec{E_3}\cdot d \vec{S_3}=0\;?$$
This is generally NOT true. If the charge is positive, the electric field points from left to right, as do both surface areas $$d\vec S_1 = \hat n dA_1$$ and $$d\vec S_3 = \hat n dA_3$$. Hence, both terms are positive (provided the charge is not zero.) -

$$\vec {E_1}\cdot d \vec{S_1}+\vec{E_2}\cdot d \vec{S_2}=0\;?$$
This is generally true. -

$$\left|d\vec A_1\cdot\hat n_1\right| \div r_1^2 =\left|d\vec A_2\cdot\hat n_2\right| \div r_2^2\;?$$

 * $$\left| \frac{d\vec A_1\cdot\hat n_1}{r_1^2}\right| =\left| \frac{d\vec A_2\cdot\hat n_2}{r_2^2}\right|$$ is generally true. The notation $$d\vec S_j = \hat n_j dA_j$$ (for $$j=1,2,3$$) is a bit confusing, and selected to compensate for the presence of different notations in the literature.  An easy way to remember that $$d\vec A_j = d\vec S_j$$ is to recognize that no other vector definition of a directed surface area is available.  As an aside, the absolute value symbols ensure that we don't care whether the electric flux is entering or exiting the Gaussian surface.  In other words, the absolute value symbols ensure that all six entities are equal:

$$ \left| \frac{d\vec A_1\cdot\hat n_1}{r_1^2}\right| \equiv \left| \frac{d\vec S_1\cdot\hat n_1}{r_1^2}\right|= $$

=\left| \frac{d\vec A_2\cdot\hat n_2}{r_2^2}\right| \equiv \left| \frac{d\vec S_2\cdot\hat n_2}{r_2^2}\right| =$$

=\left| \frac{d\vec A_3\cdot\hat n_3}{r_3^2}\right|= \left| \frac{d\vec S_3\cdot\hat n_3}{r_3^2}\right| $$

-

$$\left|d\vec A_1 \div r_1^2 \right| =\left|d\vec A_2\div r_2^2\right| \;?$$

 * $$\left|\frac{d\vec A_1 }{ r_1^2} \right| =\left|\frac{d\vec A_2 }{ r_2^2} \right|$$ is NOT generally true. However, it is true in the special case that the Gaussian surface's unit normal is parallel to the displacement vector $$\vec r$$ at both locations.

An interesting question
To illustrate the value of such "true-false" questions as a way to scaffold a mathematical proof, it would be interesting for advanced students to attempt to answer the following question:
 * Is it generally true that $$\left|\frac{d\vec A_1 }{ r_1^2} \right| =\left|\frac{d\vec A_2 }{ r_2^2} \right|$$ if and only if $$\hat n_1 = \hat n_2$$?

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 * Link to "proof" of Gauss's law that uses concepts developed by this quiz.