Investigating the 1d Equation: Charges & Field Disparity

In summary, the conversation discusses the application of the 1d equation (dE/dx = lambda/epsilon0) to two different figures. In the first case, the E-field between two charge densities is zero, while in the second case, there is a non-zero E-field due to the integration of the charge density. The speaker's intuition is proven wrong as the E-field on the left and right point in opposite directions. The 1d equation can be applied, but a negative constant needs to be added to account for the boundary conditions. The conversation concludes with understanding being reached.
  • #1
Noki Lee
4
1
Can we apply the 1d equation (dE/dx = labmda/epsilon0)dEdx=λϵ0 to the first and the second figures?
1.PNG

But, in the 2nd case,
2.png


if we integrate the charge density, some field exists between the two charge densities. Intuitively, it should be like the last figure.
What's wrong with this?
 
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  • #2
Your intuition is wrong. The E-field on the left and right point in opposite directions. This is what you get in your case (1) if you add a (negative) constant of integration so E is zero between the two charges.
 
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  • #3
phyzguy said:
Your intuition is wrong. The E-field on the left and right point in opposite directions. This is what you get in your case (1) if you add a (negative) constant of integration so E is zero between the two charges.
3.png

I mistook the intuition, did you mean this figure?

But why we can't apply the above 1D equation?
 
  • #4
Yes, I mean that figure. You can use the above 1D equation, but when you do the integration, you always have a constant of integration that you have to determine from the boundary conditions. So your graph (1) needs to have a negative constant added to it so it looks like the graph (2) in post #3. Do you understand?
 
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  • #5
phyzguy said:
Yes, I mean that figure. You can use the above 1D equation, but when you do the integration, you always have a constant of integration that you have to determine from the boundary conditions. So your graph (1) needs to have a negative constant added to it so it looks like the graph (2) in post #3. Do you understand?
I got it, thank you.
 

FAQ: Investigating the 1d Equation: Charges & Field Disparity

What is the 1d equation and how does it relate to charges and field disparity?

The 1d equation is a mathematical representation of the relationship between electric charges and the electric field they create. It describes how the electric field at a point in space is influenced by the magnitude and direction of nearby charges.

How is the 1d equation used in scientific research?

The 1d equation is used in a variety of scientific research, particularly in the fields of physics and engineering. It is used to study the behavior of electric charges and fields in different scenarios, such as in electronic circuits or in the atmosphere during a thunderstorm.

Can the 1d equation be applied to real-world situations?

Yes, the 1d equation can be applied to real-world situations. It is a fundamental equation in electromagnetism and is used to understand and predict the behavior of electric charges and fields in various systems and environments.

Are there any limitations to the 1d equation?

Like any mathematical model, the 1d equation has its limitations. It assumes that charges and fields are present in a one-dimensional space, which may not always be the case in real-world situations. Additionally, it does not take into account certain factors such as the effects of relativity or quantum mechanics.

How can the 1d equation be solved and what are the units of the solution?

The 1d equation can be solved using various mathematical techniques, such as integration or solving for unknown variables. The units of the solution will depend on the specific values and units used in the equation, but it will typically be in units of electric field (N/C or V/m).

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