Potential energy for a dipole between 2 infinitely large charged sheets

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SUMMARY

The discussion centers on calculating the potential energy, torque, and net force on a dipole consisting of charges +/- e separated by 220 nm, placed between two infinitely large charged sheets with a surface charge density of 125 µC/m². The maximum potential energy of the dipole is determined to be 3.22 x 10^-14 J, achieved when the dipole is oriented with its negative charge facing the negatively charged sheet. The correct approach to find the electric field between the sheets involves using Gauss's law rather than the initially referenced equation. The torque and net force calculations were also discussed but require further clarification on the electric field strength.

PREREQUISITES
  • Understanding of dipole moment and its calculation (p = qd)
  • Familiarity with electric fields generated by charged sheets (E = λ / (2ε))
  • Knowledge of potential energy in electric fields (U = -pEcos(φ))
  • Basic principles of Gauss's law for electric fields
NEXT STEPS
  • Learn how to apply Gauss's law to calculate electric fields from charged sheets
  • Study the concept of torque on dipoles in electric fields
  • Explore the implications of dipole orientation on potential energy and torque
  • Investigate the relationship between surface charge density and electric field strength
USEFUL FOR

Students and educators in physics, particularly those focusing on electromagnetism, as well as anyone involved in advanced problem-solving related to electric fields and dipoles.

Emethyst
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Homework Statement


A dipole consisting of charges +/- e 220 nm apart is placed between two very large (essentially infinite) sheets carrying equal but opposite charge densities of 125 uC/m^2.

a) What is the maximum potential energy this dipole can have due to the sheets, and how should it be oriented relative to the sheets to attain this value?

b) What is the maximum torque the sheets can exert on the dipole, and how should it be oriented relative to the sheets to attain this value?

c) What net force do the two sheets exert on the dipole?


Homework Equations


U = -pEcos(\phi)
p = qd
E = \lambda/2\pi\epsilonx
where \lambda is the linear charge density, \epsilon is the permittivity of free space, and x is a distance for a point P from the sheet.
\sigma = q/A (surface charge density)


The Attempt at a Solution


I can see from the start that once I acquire a) the rest of the question should go smoothly. Where I am stuck is trying to calculate the initial electric field between the infinite sheets that the dipole lies in. What I tried to do was first find the linear charge density from the given surface density, arriving at a value of 11.2 uC/m by simply taking the square root of the 125 uC/m^2.

Next I treated each sheet as essentially lying where the point charges of the dipole lie (aka giving a distance of 220 nm between each sheet). With the distance found I then plugged this along with all other needed values into the electric field equation provided (the equation for the electric field strength for a point P a distance x away from an infinitely large sheet I found in my textbook).

From there I then multiplied this value by the dipole moment to arrive at an answer of 3.22 x 10^-14 J for the potential energy. I already know for maximum potential energy the dipole should be oriented so that its negative charge faces the negatively charged sheet (dipole moment should be in the opposite direction of the electric field, giving an angle of 180 to make cos\phi = -1 and thus cancel out the negative from the potential energy equation). My concern is that I think I am making too many assumptions (ex. about the distance between the two sheets) and am ultimately calculating the external electric field wrong. If someone could tell me if I am right or wrong, and if wrong point me in the right direction it would be greatly appreciated.
 
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I think you are calculating the electric field between the two sheets wrong? What is that equation E = \lambda / 2 \pi \epsilon x ? That's not the equation for the electric field between infinite parallel sheets.

You can find the electric field due to an infinite charged sheet by using the Gauss law. Then you can find the electric field between two of them by adding the components of the electric field made by each one of the sheets.
 

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