Electric Field/Electric Potential (Gradient Notation)

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Homework Help Overview

The discussion revolves around the notation and interpretation of the electric field and electric potential, specifically focusing on the gradient notation used in expressing the relationship between these two concepts.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to clarify the notation for the electric field derived from the electric potential using gradient notation, questioning the correctness of expressing the electric field as a vector derived from the potential.
  • Some participants suggest sticking to traditional notation for clarity, while others question the implications of certain notations that may suggest the potential is a vector.
  • Further inquiries are made regarding the validity of rewriting the electric field in terms of partial derivatives with respect to multiple variables.

Discussion Status

Participants are actively exploring the nuances of notation and its implications. Some guidance has been offered regarding the appropriateness of certain expressions, with a recognition of the potential confusion that may arise from non-standard notation. Multiple interpretations of the gradient and its representation are being discussed.

Contextual Notes

There is an ongoing examination of the definitions and properties of scalar and vector fields, particularly in the context of electric potential and electric field relationships. The discussion is framed within the constraints of formal definitions in physics.

PFStudent
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Homework Statement



Hey,

I have a question about Electric Field/Electric Potential gradient notation.

Since,

<br /> {\vec{E}} = {-}{\nabla}{V(r)}<br />

Which reduces to,

<br /> \vec{E} = {-}{\nabla}{V(x, y, z)}<br />

When expanded is,

<br /> \vec{E} = {-}{\left[{\frac{\partial[V]}{\partial{x}}}{\hat{i}} + {\frac{\partial[V]}{\partial{y}}}{\hat{j}} + {\frac{\partial[V]}{\partial{z}}}{\hat{k}}\right]}<br />

So using partial derivative notation can I write,

<br /> {\vec{E}} = {-}{\vec{V}&#039;_{xyz}}<br />

So, is the above correct notation?

The reason I am hesitant is, because formally the gradient is defined as a vector operator that takes a scalar field (such as the electric potential) and changes it to a vector field (such as the electric field) through: partial differentiation with the addition of unit vectors (\hat{i}, \hat{j}, \hat{k}).

However, writing it as below sort of implies the potential is a vector (which it isn't), but gives the impression that it is because of how the gradient is defined.

<br /> {\vec{E}} = {-}{\vec{V}&#039;_{xyz}}<br />

So, is the above notation correct?

-PFStudent
 
Last edited:
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PFStudent said:
However, writing it as below sort of implies the potential is a vector (which it isn't), but gives the impression that it is because of how the gradient is defined.

<br /> {\vec{E}} = {-}{\vec{V}&#039;_{xyz}}<br />

So, is the above notation correct?

-PFStudent

I wouldn't use it. I would just leave it as:

<br /> {\vec{E}} = {-}{\nabla}{V(r)}<br />

Or

<br /> {\vec{E}} = {-}{\nabla}{V}<br />
 
PFStudent said:
<br /> {\vec{E}} = {-}{\vec{V}&#039;_{xyz}}<br />

So, is the above notation correct?

No, it is not correct. That is, there is no notation I know of that looks like that that is defined as the gradient of a scalar field.

As the above poster says, there is nothing wrong with \vec{E}=-\nabla V
 
Hey,

Yea, thanks for the input, I can see why that notation,

<br /> {\vec{E}} = {-}{\vec{V}&#039;{xyz}}<br />

is wrong. Since, we are adding the components of a vector that is not the same as taking the partial derivative of a function with respect to each of the variables.

Since, all the gradient is doing is the following,

<br /> \vec{E} = {-}{\nabla}{V(x, y, z)} = {-}{\left[{\frac{\partial}{\partial{x}}{\left[V\right]}} + {\frac{\partial}{\partial{y}}}{\left[V\right]}} + {\frac{\partial}{\partial{z}}}{\left[V\right]}}\right]}{\hat{r}}<br />

Thanks,

-PFStudent
 
Hey,

I've been thinking about this and I have a follow up question.

Since,

<br /> \vec{E} = {-}{\nabla}{V(r)} = {-}{\left[{\frac{\partial}{\partial{x}}{\left[V\right]}} + {\frac{\partial}{\partial{y}}}{\left[V\right]}} + {\frac{\partial}{\partial{z}}}{\left[V\right]}}\right]}{\hat{r}}<br />

and also,

<br /> E = {-}{\frac{\partial}{\partial{r}}}{\left[{V(r)}\right]}<br />

So then,

<br /> \vec{E} = {-}{\nabla}{V(r)} = {-}{\frac{\partial}{\partial{r}}}{\left[{V(r)}\right]}{\hat{r}}<br />

Now can I rewrite the above as below?

<br /> \vec{E} = {-}{\frac{\partial}{\partial{(x, y, z)}}}{\left[{V(x, y, z)}\right]}{\hat{r}}<br />

Which for {E} can also be written as,

<br /> {E} = {-}{\frac{\partial}{\partial{(x, y, z)}}}{\left[{V(x, y, z)}\right]}<br />

So, is the notation for the above two equations correct?

Thanks,

-PFStudent
 

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