Electrodynamics Continuity Equation

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SUMMARY

The discussion centers around the Continuity Equation in Electrodynamics, specifically the equation ∇J = -∂ρ/∂t, which represents local charge conservation as defined by David Griffiths. Participants clarify that the correct formulation should be ∂ρ/∂t = ∇·J, and they explain its physical meaning through the analogy of water flow. The integral form of the equation, which involves integrating over a volume and applying the divergence theorem, is emphasized as a crucial aspect for understanding the relationship between charge density and current density.

PREREQUISITES
  • Understanding of vector calculus, particularly divergence and integrals.
  • Familiarity with the concepts of charge density (ρ) and current density (J).
  • Knowledge of the divergence theorem in mathematical physics.
  • Basic principles of Electrodynamics as outlined in Griffiths' textbook.
NEXT STEPS
  • Study the integral form of the Continuity Equation in detail.
  • Learn about the divergence theorem and its applications in Electrodynamics.
  • Explore charge conservation principles in various physical systems.
  • Review examples of current density in fluid dynamics for better conceptual understanding.
USEFUL FOR

Students preparing for exams in Electrodynamics, educators teaching physics concepts, and anyone seeking to deepen their understanding of charge conservation and current density relationships.

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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