B Different formulas for electric flux

AI Thread Summary
The discussion highlights discrepancies in electric flux formulas between different textbooks, specifically Tipler and Hayt. Tipler defines electric flux through a surface using the electric field (E), while Hayt presents it in terms of electric flux density (D) over an enclosed surface. Participants note the importance of distinguishing between electric flux and electric flux density, suggesting that the term "displacement flux density" might be more appropriate for D. The conversation also emphasizes that while the definitions differ, they can be reconciled through unit consistency, as both ultimately relate to charge (Q). Overall, the complexities of these definitions reflect deeper principles in electromagnetism and the importance of clarity in terminology.
Alex Schaller
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I noticed that in some textbooks (Physics - Tipler) the electric flux formula is different than in other textbooks (Engineering Electromagnetics -W. Hayt)

Which one should we use?
electric flux stated differently.jpg
 
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Tipler gives the standard definition of flux through a surface. Use that one.

Hayt seems to be talking about the total flux through an enclosed surface. Look up Gauss' law in Tipler for more.
 
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Read this: Gauss's Law
 
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Be careful to distinguish between electric flux and electric flux density.
 
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Doc Al said:
Be careful to distinguish between electric flux and electric flux density.
Yes, you are correct.

Hayt conveys "electric flux" as the integration of "electric flux density D" over a surface, whereas Tipler conveys "electric flux" as the integration of "electric field E" over a surface.
Hayt.jpg
 

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Because electric flux is defined as ##~ d \Phi_e = \mathbf {E} \cdot d\mathbf {S}~##, it is very reminiscent that the electric field strength or electric field intensity ##~E = \frac {\Phi_e} {S~cos\phi}~## itself represents the electric flux density, but on the other hand, the electric flux density is defined as ##~\mathbf {D}=\epsilon\mathbf {E} ~ ~##(there is an extra symbol##~\epsilon~## before ## \mathbf E ##) , which is really a bit confusing to me.😓

Perhaps we better not call ## ~\mathbf {D}~## the electric flux density, the name electric displacement field may be more suitable for it.

https://en.wikipedia.org/wiki/Electric_flux
https://en.wikipedia.org/wiki/Electric_displacement_field
 
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Thanks for your reply Alan,
I agree with you, perhaps D should be called "displacement flux density" or "displacement density" and not "electric flux density".

On the other hand, flux as per Hayt (Φ = Q) is simpler to understand, but does not yield the same equation as flux according to Tipler (Φ = Q/ε0).

Maybe we should send a suggestion to the editor of Hayt's textbook to look it over?
 
Alex Schaller said:
Maybe we should send a suggestion to the editor of Hayt's textbook to look it over?

Looking at it from another angle, this matter is actually not a big deal. When we express the same thing, we will use different units. For example, the unit of weight can be mg, kg or pound, etc., and the unit of distance can be meter, kilometer or light-year, etc., so just indicate the unit to avoid misunderstanding.

The unit of electric flux based on ## ~ \Phi_e = E S~cos\phi~ ## is volt meters (Vm).

Because the unit of ## ~\epsilon~## is ## \frac {C} {Vm} ~##, the unit of electric flux based on ## ~ \Phi_e =DS~cos\phi = ~\epsilon~E S~cos\phi~ ## is ## \left(\frac {C} {Vm} \right) \left( Vm \right) = C~##. That's why I mentioned earlier that I prefer the expression ##~\Phi_e =Q ~##, which seems to be more concise and beautiful in my opinion.

On the other hand, this is also in line with symmetry.
## ~ \Phi_e = D S~cos\phi~ ##, where D is called the electric flux density
## ~ \Phi_m = B S~cos\phi~ ##, where B is called the magnetic flux density
 
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Thanks Alan!

Talking about symmetry I thought B was more related to E, as H was more related to D (both E and B take into account all the charges present -free and bond-, whereas H and D only consider the free charges).
 
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Indeed, ##\vec{E}## and ##\vec{B}## belong together and ##\vec{D}## and ##\vec{H}##. This becomes very clear in the more consistent manifestly covariant relativistic formulation of electrodynamics, where ##\vec{E}## and ##\vec{B}## are the 6 independent components of an antisymmetric four-tensor ##F_{\mu \nu}## and ##\vec{D}## and ##\vec{H}## of another such tensor ##D_{\mu \nu}##.
 
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