Electrodynamics Continuity Equation

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Homework Help Overview

The discussion revolves around the continuity equation in electrodynamics, specifically its mathematical formulation and physical interpretation. The original poster is seeking clarity on the concept of charge conservation as expressed by the equation ∇J = -∂ρ/∂t.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the physical meaning of the continuity equation, with one suggesting an analogy involving water flow to illustrate the concept of current density. Others question the accuracy of the equation presented and seek interpretations of its implications.

Discussion Status

There is an ongoing exploration of the continuity equation, with participants providing alternative perspectives and analogies. Some have pointed out potential typographical errors in the equation, while others are attempting to clarify the relationship between charge flow and current.

Contextual Notes

Participants are navigating through definitions and interpretations, with an emphasis on understanding the continuity equation's implications in the context of charge conservation. There is a noted lack of consensus on certain interpretations, particularly regarding the relationship between charge flow and current.

CSOleson
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Homework Statement


I am currently studying for a quiz and then following a test in my Electrodynamics test. Right now I am struggling to define the following:
Continuity equation and its physical meaning

Homework Equations


The Continuity Equation is given as the following:
∇J=-∂ρ/∂t

The Attempt at a Solution


There is no solution, I just know that it is the mathematical statement of a local charge conservation (defined by Griffiths). So what is the physical meaning? Can someone help me wrap my head around this concept?
 
Last edited:
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You have a typo. It should be
$$\frac{\partial\rho}{\partial t} = \nabla\cdot \vec{J}.$$ It might be easier for you to understand in integral form. If you integrate the equation over a volume V bounded by a closed surface S, you get
$$\frac{\partial}{\partial t}\int_V \rho\,dv = \int_V (\nabla\cdot \vec{J})\,dv = \oint_S \vec{J}\cdot d\vec{S}$$ where the last equality is the divergence theorem. Can you interpret that equation?
 
I am in the same position as you my friend. but I think that the closest I could physically interpret it is if I use an analogy of water being displaced. A drop of water can be considered as a current density J and they are saying if the drop of water begins to flow away from its point of rest, then as you sum up all the portions that are flowing away between the time it flows away then you would get the same flow rate as if the entire drop of water were to move from one point to another in the same time frame. If I am lacking in my understanding, can someone please steer me in the right direction.
 
Last edited by a moderator:
vela said:
You have a typo. It should be
$$\frac{\partial\rho}{\partial t} = \nabla\cdot \vec{J}.$$ It might be easier for you to understand in integral form. If you integrate the equation over a volume V bounded by a closed surface S, you get
$$\frac{\partial}{\partial t}\int_V \rho\,dv = \int_V (\nabla\cdot \vec{J})\,dv = \oint_S \vec{J}\cdot d\vec{S}$$ where the last equality is the divergence theorem. Can you interpret that equation?

Is it describing the flowing charge produces a current?
 
No. A flow of charge is by definition a current.
 

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