Maxwell's Equations: Symbols & Understanding

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SUMMARY

This discussion focuses on understanding Maxwell's equations, specifically the differential forms involving the del operator. The del operator represents operations in vector calculus, notably divergence and curl, which are essential for analyzing electric fields. The divergence measures the flow of a vector field into or out of a point, while curl quantifies the rotational aspect of the field. The conversation also highlights the differences between integral and differential forms of Maxwell's equations, noting that while integral forms are often used for Gauss' law, differential forms are preferred for proofs related to electromagnetic waves and energy in fields.

PREREQUISITES
  • Basic understanding of Electricity and Magnetism
  • Familiarity with Calculus, particularly vector calculus
  • Knowledge of integral and differential forms of equations
  • Experience with vector fields and operations like dot and cross products
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  • Study the del operator in various coordinate systems, including spherical coordinates
  • Learn how to compute divergence and curl for different vector fields
  • Explore the applications of Gauss' law in both integral and differential forms
  • Investigate electromagnetic wave propagation and its derivation from Maxwell's equations
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Students and professionals in physics, electrical engineering, and applied mathematics who seek a deeper understanding of Maxwell's equations and their applications in electromagnetism.

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I was curious about the famous Maxwell's equations, and decided, perhaps foolishly, to learn them myself. I know basic Electricity and Magnetics with Calculus, so I figured it was the next logical step. I understood the integral forms of Maxwell's equations, but I got completely lost when I saw the upside down deltas in the differential forms of the equations. Could someone tell me what they stand for and/or what mathematical operation they entail?
 
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That's called the del operator, and it is a concise way of representing a number of different operations in vector calculus. Maxwell's equations use two of these operations: divergence and curl. The divergence of a vector field is a scalar field that rougly measures how much the field is flowing into or out of each point. The curl is a vector field that measures how much it curls around each point, with the magnitude of the vector representing the magnitude of the curl and the direction representing the direction of flow (the same way the angular momentum vector works). To actually compute these quantities, the del operator can be written as \frac{d}{dx}\hat x+\frac{d}{dy}\hat y+\frac{d}{dz}\hat z, and then the appropriate operations (dot or cross products) can be performed on the field, substituting the differential operation for multiplication. This only works in cartesian coordinates, and in other systems (eg, spherical), the del operator is written differently.
 
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So, just to clarify, if you had the electric field as some vector function...you'd take the derivative of that vector, then dot or cross that derivative with the original electric field function, as shown here?

deloperator(E)= E' x E

Where E=electrive field (vector), E' = the derivative of the electric field.

Or have I just horribly confused it?

Also, is there any advantage to using the differential forms over integral forms?

EDIT: By derivative, I mean take the derivative of each vector component with respect to that components axis.
 
No, I'm sorry, I should have been clearer. You treat the del as if it were a vector. So if the vector field has components Ex, Ey, and Ez, then dotting the del (taking the divergence) would look like this:

\nabla \cdot E= (\frac{d}{dx} \hat x + \frac{d}{dy} \hat y + \frac{d}{dz} \hat z) \cdot (E_x \hat x + E_y \hat y +E_z \hat z)

= \frac{d}{dx} E_x + \frac{d}{dy} E_y + \frac{d}{dz} E_z = \frac{dE_x}{dx} + \frac{dE_y}{dy} + \frac{dE_z}{dz}

Curl is a little more complicated, but it's the same idea. As for the usefulness of each form, it all depends on what you're trying to do. Gauss' law, for example, is usually used in its integral form for most problems. I would say that most proofs and derivations of things like EM waves and the energy and momentum stored in the fields are easier using the differential forms of the equations.
 
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Thanks a 3x10^8 ;) .
 

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