Griffiths Problem 3.34: Analyzing Induced Charge & Grounded Plate

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SUMMARY

The discussion centers on Griffiths' Problem 3.34 regarding induced charge on a grounded conducting plate. Participants clarify that the grounded plate maintains a potential of zero, necessitating an induced charge to achieve this state. The total induced charge on the grounded plane is confirmed to be -q, as derived from Gauss's law. The conversation also touches on the differential equation related to the motion of the charge above the plate, emphasizing the need to equate forces for proper analysis.

PREREQUISITES
  • Understanding of electrostatics, particularly induced charge concepts
  • Familiarity with Griffiths' "Introduction to Electrodynamics"
  • Knowledge of Gauss's law and its applications
  • Basic proficiency in solving differential equations
NEXT STEPS
  • Study the method of images in electrostatics as outlined in Griffiths' textbook
  • Learn how to apply Gauss's law to various geometries
  • Explore differential equations related to electrostatic forces
  • Review grounding effects on potential and charge distribution in conductors
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Students of electromagnetism, physics educators, and anyone seeking to deepen their understanding of electrostatic principles and grounded conductors.

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Homework Statement


This question refers to Griffiths E and M book.

If they had not told me that the charge moves, I would have guessed that it just sits there since it seems like there is nothing to exert a force on it. Am I supposed to calculate the induced charge on the conducting plate? How do I use the fact that the plate is grounded? That means that the potential on the plate is 0 just like at infinity, but doesn't that imply there is no charge on the plate either?


Homework Equations





The Attempt at a Solution

 
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No, the charge on the plate is needed to keep it at V=0.
The charge is supplied by the ground.
Read the part in Griffith's about images for grounded plates.
 
pam said:
No, the charge on the plate is needed to keep it at V=0.
The charge is supplied by the ground.
Read the part in Griffith's about images for grounded plates.

A related question: on page 123, Griffiths says "Evidently the total induced charge on the plane is -q, as (with the benefit of hindsight) you can perhaps convince yourself that it had to be."

I cannot convince myself unfortunately. How do you know this a priori? Is it related to the fact that the plate is grounded? Would it be different if the plate were not grounded?
 
And also when I try to apply eqn 3.12 to this problem I get a differential equation which I have no idea how to solve:

\ddot{z} = C/z^2

where C is a constant. What am I doing wrong?
 
1. The image charge is -q. By Gauss's law, that has to equal the induced surface charge on the grounded plane.

2. Use dv/dt=v(dv/dx).
 
ehrenfest said:

Homework Statement


This question refers to Griffiths E and M book.

If they had not told me that the charge moves, I would have guessed that it just sits there since it seems like there is nothing to exert a force on it. Am I supposed to calculate the induced charge on the conducting plate? How do I use the fact that the plate is grounded? That means that the potential on the plate is 0 just like at infinity, but doesn't that imply there is no charge on the plate either?

Homework Equations


The Attempt at a Solution


Calculate the force on the charge at a height 'x' above the plane and equate it with the equation of motion of the charge 'q'.
 

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