Finding scalar potential from E-field and vector potential

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SUMMARY

The discussion focuses on calculating the scalar potential \( V \) from a given electric field \( \mathbf{E} \) and vector potential \( \mathbf{A} \). The electric field is defined as \( \mathbf{E}(t, \vec{r}) = \frac{\kappa}{\varepsilon_0} \begin{bmatrix} ctx + x^2 - y^2 \\ cty + y^2 \\ ctz + z^2 - y^2 \end{bmatrix} \) and the vector potential is \( \mathbf{A} = \frac{\kappa t}{\varepsilon_0} \begin{bmatrix} y^2 \\ 0 \\ y^2 \end{bmatrix} \). The relationship \( \mathbf{E} = -\nabla V - \frac{\partial \mathbf{A}}{\partial t} \) is established, leading to the need for expressing \( V \) in terms of its derivatives. The user seeks clarification on isolating \( V \) and deriving its general form from the equations provided.

PREREQUISITES
  • Understanding of vector calculus, specifically gradient operations.
  • Familiarity with electric fields and potentials in electromagnetism.
  • Knowledge of partial differential equations and their applications.
  • Experience with vector potentials and their relationship to electric fields.
NEXT STEPS
  • Study the derivation of scalar potentials from electric fields in electromagnetism.
  • Learn about the mathematical implications of the gradient operator in three-dimensional space.
  • Explore the relationship between vector potentials and electric fields in Maxwell's equations.
  • Investigate methods for solving partial differential equations related to electromagnetic fields.
USEFUL FOR

Students and professionals in physics, particularly those focusing on electromagnetism, as well as anyone involved in solving problems related to electric and vector potentials.

Denver Dang
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Homework Statement


Hi.

This one I really am lost on :/
In my mind it seems rather easy, but I still can't figure it out.
I have been given the E-field:
<br /> \mathbf{E}\left( t,\,\,\vec{r} \right)=\frac{\kappa }{{{\varepsilon }_{0}}}\left[ \begin{matrix}<br /> ctx+{{x}^{2}}-{{y}^{2}} \\<br /> cty+{{y}^{2}} \\<br /> ctz+{{z}^{2}}-{{y}^{2}} \\<br /> \end{matrix} \right]<br />
And then I have calculated the vector potential, which gives:
\mathbf{A}=\frac{\kappa t}{{{\varepsilon }_{0}}}\left[ \begin{matrix}<br /> {{y}^{2}} \\<br /> 0 \\<br /> {{y}^{2}} \\<br /> \end{matrix} \right]<br />
And now I need to calculate the scalar potential

Homework Equations


I'm thinking this one:
\mathbf{E}=-\nabla V-\frac{\partial \mathbf{A}}{\partial t}

The Attempt at a Solution


My problem is, that I'm not entirely sure about what to do with the scalar potential V.
Taking the derivative of A is no problem, and adding E and A together is easy as well. But how is it get the scalar potential to stand alone ? Differentiate with \nabla on both sides doesn't make sense to me.

I'm guessing it's pretty simple, but again, at the moment, I'm kinda lost :/

So any help would be appreciated.Thanks in advance.
 
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You should be able to write out three partial differential equations (expressing ∇V = some vector). If one of those equations looks like, say, ∂V/∂x = f(x), what could you write down as the general form of V?
 
i would write out i=x, y, z and consider them all at once.

$$E_i = -\frac{\partial}{\partial x^i}\phi -\frac{\partial A_i}{\partial t} $$
 

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