Del dot E equals 0 and Del dot B equals 0, both in a vacuum

In summary: I see. So outside of a vacuum, electric fields have a divergence?Yes, electric fields have a divergence.
  • #1
rockyshephear
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0
So given the common explanation here for Del dot B equals 0 to be "There are no magnetic monopoles.", since the title indicates that the equations in a vacuum have the same form, would the meaning of Del dot E = 0 mean that "There are no ELECTRIC monopoles?"...which we assume to be false. Wherein lies the confilct?
 
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  • #2
Both statements are true in a vacuum, because by definition there are no electric monopoles in a vacuum. If there were electric monopoles it wouldn't be a vacuum. In general
[tex]\nabla\cdot \vec{E} = \frac{\rho}{\epsilon_{0}}[/tex]
This applies even when electric monopoles are present.
 
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  • #3
Do you mean you can't have electric monopoles in a vacuum because a vacuum can have no charges in them?
 
  • #4
Yes, the definition of a vacuum is a place where there is no matter. Charges are made of matter, so a vacuum can contain no charge.
 
  • #5
You also cannot have magnetic monopoles (if they exist) in a vacuum since that would also imply the presence of matter, right?
 
  • #6
That's kind of a silly equation. Kind of like saying there is no laminar flow in a vacuum. There's no anything in a vacuum! lol I wonder why it was even stated?
 
  • #7
It seems silly at first, but there are electric and magnetic fields in a vacuum even though there is no matter. This equation is important, for instance, in studying how an electromagnetic wave propagates in a vacuum.
 
  • #8
Oh, so you can have a point charge outside the defined vacuum and it permeates into the vacuum?
 
  • #9
Yes, the electric field of a point charge will permeate all of space. If there is only 1 point charge, then in any region that does not include that charge,
[tex]\nabla\cdot\vec{E} = 0 [/tex]
but that is not true at the location of the charge.
 
  • #10
Not sure what you mean about "but that is not true at the location of the charge. Is it semantics to say there is not electric field at the exact charge point? I guess the electric field =0 there, right? But given that, then if there were another charge point, it's field woulcd be exactly at the first chage points position.
 
  • #11
Are you a famous physicist? You have a famous physicist type of name.
 
  • #12
rockyshephear said:
Not sure what you mean about "but that is not true at the location of the charge."

Sorry if that was unclear. I'll restate it like this: draw any box in space. If it doesn't contain the charge, then it is a vacuum and [tex]\nabla\cdot\vec{E} = 0[/tex] everywhere inside. If it does contain the charge, then it is not a vacuum and that equation does not apply everywhere inside.

It's probably best not to think of the electric field as being 0 at the location of a point charge, just undefined. Certainly [tex]\nabla\cdot\vec{E}[/tex] is not defined there.

rockyshephear said:
Are you a famous physicist? You have a famous physicist type of name.
No, I'm not actually Leonhard Euler. He lived in the 1700's and was one of the greatest mathematicians of all time. I just chose my name in honor of him.
 
  • #13
I wish to for sake of learning, argue that Del dot E is not zero inside the box, because in my limited knowledge I would say that the divergence of an electric field is a function of the interacting waves of many point charges and millions could be interacting inside a vacuum box. How would you respond to that? I though his name sounded familiar. lol
 
  • #14
Yes, millions of charges outside the box could be influencing the field in the vacuum box, but the divergence would still be 0. The easiest way to see this is that if I have a lot of charges outside the box, call them q1, q2 ... q1000000, the total electric field at any point is the sum of the electric fields resulting from each charge alone (superposition principle):
[tex]\vec{E}_{TOT} = \vec{E}_{1} + \vec{E}_{2} + ... + \vec{E}_{1000000}[/tex]
The divergence is also a linear operator, so
[tex]\nabla\cdot\vec{E}_{TOT} =\nabla\cdot \vec{E}_{1} + \nabla\cdot\vec{E}_{2} + ... + \nabla\cdot\vec{E}_{1000000}[/tex]

You can fairly easily show that the divergence of the field of one charge is 0. That applies to all of the charges, so
[tex]\nabla\cdot\vec{E}_{TOT} = 0 + 0 + ... + 0 = 0[/tex]
 
  • #15
Hmmm...sounds good but I'm still not getting divergence. I see it as the rate of change of an electric field and inside the box you've got flux lines (like in those 2D drawings of charge interactions) and at one point in the box more lines converge, more divergence and at other points in the box, less lines converge, less divergence. If what you say in true then you cannot have divergence in a vacuum. So outside of a vacuum, how do you demonstrate divergence? Sorry for being terminally thick on this but it's really difficult to conceptualize.
 
  • #16
rockyshephear said:
I see it as the rate of change of an electric field and inside the box you've got flux lines (like in those 2D drawings of charge interactions) and at one point in the box more lines converge, more divergence and at other points in the box, less lines converge, less divergence.

I'm sorry but I can't quite understand this. You don't have more divergence at some points in a vacuum and less at others. It is zero everywhere.

A way to picture divergence is this: Draw a small region in space and calculate how much electric field enters and how much leaves. Let the size of this box shrink to 0. If more electric field is leaving, there is positive divergence. If more is entering, there is negative divergence.

The divergence due to a single charge is 0, so the amount entering and leaving are in balance for each charge. Add them all together and they are still in balance.
 
  • #17
I think this is the most difficult concept to grasp. By your statement, you never have divergence NOT equal zero unless an electric field enters a closed 2D surface and vanishes magically. I don't think electric fields just vanish. And if they don't vanish, they proceed thru the surface, so you always have zero divergence. Correct me if I'm wrong here but maybe my example will clear up my inability to grasp this.
 
  • #18
That's not quite right. If the electric field entered the box and disappeared, the divergence would NOT be zero, because it comes in but doesn't go out. Think of the vector field that describes the velocity of a liquid. If you draw any closed surface, the amount of liquid coming into the surface has to equal the amount leaving. This means the divergence of the velocity field is 0. So too with the electric field.
 
  • #19
rockyshephear said:
I think this is the most difficult concept to grasp. By your statement, you never have divergence NOT equal zero unless an electric field enters a closed 2D surface and vanishes magically. I don't think electric fields just vanish. And if they don't vanish, they proceed thru the surface, so you always have zero divergence. Correct me if I'm wrong here but maybe my example will clear up my inability to grasp this.

The solution to this is that for a non-zero divergence, you must have a source or sink inside the volume. This is why they describe divergence as a measure of sources/sinks. The differential and integral forms of Maxwell's equations are equivalent. One can think of the differential form of Gauss' Law as being the limit of the integral form as the enclosed volume of integration goes to zero. Thus, the divergence of the electric field is zero everywhere except for the exact points in space where we have a charge, which acts as a source.
 
  • #20
rockyshephear said:
I think this is the most difficult concept to grasp. By your statement, you never have divergence NOT equal zero unless an electric field enters a closed 2D surface and vanishes magically. I don't think electric fields just vanish. And if they don't vanish, they proceed thru the surface, so you always have zero divergence. Correct me if I'm wrong here but maybe my example will clear up my inability to grasp this.

Dude, seriously. Maxwell's equations are MATHEMATICALLY derived from VECTOR CALCULUS mapped to a physical situation. Saying Del dot B is a silly law is just retarded. Maxwell's equation are actually used, using MATH to SOLVE PROBLEMS. And each one is of extreme importance. One does not work without the other, in those 4 equations is EVERYTHING physical about classical EM. All the rest of classical EM is just a developed mathematical toolbox to help with certain types of problems (usually with high symmetry).

P.S. as has been stated, Euler was one of the best mathematicians ever, not a physicist. There is a joke in math: "Why are there not many things named after Euler?", "Because in math things often get named after the SECOND person who discovered them and the first person was always Euler".
 
  • #21
So let's recap. In a vacuum, divergence is zero becuase electric and magnetic 'radiation' or call it what you will, goes right thru it and out the other side. If if there were a point charge in the box, the divergence would not be zero. So, now how does all this equate to Del Dot B =0 I don't see a box anywhere. lol I assume that Del Dot B =0 means the divergence of B is zero no matter in a vacuum or outside of one. Could one consider a magnet as a 'source' and a 'sink' since it kind of leaves the soure and enter the sink? I guess so, but they cancel each other out, right?
So doesn't Del Dot B = 0 really mean
if you take the smallest dipole known, you will see magnetic flux leaving it and entering it, so the source equals the sink and as such the divergence =0. And in this case the dipole is actually the box we referred to. Right?
 
  • #22
Not 'radiation' but fields. Radiation is traveling electromagnetic (or other particles depending upon what you mean) waves.

In the differential form, the box is infinitesimally small, it is a point. The basic source of a magnetic field is a dipole, which has both the features of a source and a sink since the same number of effective field lines will exit a volume enclosing the dipole source as those that enter it. Because of this, it is neither a net source or a net sink (in terms of divergence) and thus has a zero divergence. Since the magnetic field is derived solely of dipole sources, it's divergence will always be zero regardless of the environment.
 
  • #23
Ok. One down. Anyone care to quiz me on this? I am sure I have Del Dot B down as far as describing it. But the math is something different?
What is see is a cross product operation combined with Nabla. I've only learned how to do cross product calculations with two vectors. And I've learned that if the answer is 0, then the two vectors are 90 degrees apart (if I remember correctly). So since I see a cross product operator, I would assume that something in Del Dot B = 0 has to have two vectors that are 90 degrees apart. Is there no correlation?
 
  • #24
Nabla is an operator, it is not a vector. If you see nabla involved in anything you need to look up what it translates too. Even if it is something simple like a divergence, the divergence operator is different depending upon the coordinate system you are using. If you saw:

[tex]\nabla\times\nabla\times f(x,y,z)[/tex]

This is a valid operation and results in what is called a dyadic. A dyadic is a three rank tensor, a 3x3 matrix, with elements like

[tex]\hat{x}\hat{x},\hat{x}\hat{y},\hat{x}\hat{z}[/tex]

would be the top row for example. The idea being that this dyadic will relate a vector to a vector. That is, the dot product to the left or right of the dyad with a vector results in a vector as opposed to a dot product between vectors that results in a scalar.
 
  • #25
wow, the dyadic wears a lot of hats. Ok, I'm fried for a while. Thanks for all the help. Feel free to delete any of the questions to clear up space.
 

1. What does "Del dot E equals 0 and Del dot B equals 0, both in a vacuum" mean?

Del dot E and Del dot B are equations that represent the divergence of the electric and magnetic fields, respectively. In a vacuum, these equations state that the fields do not have any sources or sinks, meaning they are constant and have a net flux of zero.

2. Why is it important that these equations hold true in a vacuum?

In a vacuum, there are no external sources or influences on the electric and magnetic fields. Therefore, these equations are fundamental principles that govern the behavior of these fields in the absence of any other factors. This allows scientists to make accurate predictions and calculations in various fields such as electromagnetics and optics.

3. How do these equations relate to Maxwell's equations?

Del dot E equals 0 and Del dot B equals 0 are two of the four Maxwell's equations, specifically the equations for Gauss's law and Ampere's law with no current, respectively. These equations describe the behavior of electric and magnetic fields in a vacuum and are essential in understanding the fundamentals of electromagnetism.

4. Can these equations be applied in non-vacuum environments?

Yes, these equations can also be applied in non-vacuum environments, but they may be modified to account for external sources or influences on the fields. For example, in the presence of a charge or current, the Del dot E and Del dot B equations would no longer equal zero.

5. What are the implications of these equations for electromagnetic waves?

In a vacuum, these equations show that electromagnetic waves can propagate indefinitely without any external sources or influences. This is known as the principle of electromagnetic wave propagation and is a fundamental concept in understanding the behavior of light and other electromagnetic radiation.

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