chrisych
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Does anyone know how to calculate these questions?
The discussion revolves around calculating electric field strength and potential differences related to point charges. Participants are exploring the relationships between electric field, charge, and work done, as well as the vector nature of electric fields.
Some participants have provided guidance on using vector components and have pointed out potential errors in reasoning. Multiple interpretations of the problem are being explored, particularly regarding the calculation of resultant electric fields.
There is an emphasis on showing work and identifying where participants are struggling, as well as a reminder to consider the vector nature of electric fields. The discussion includes specific values and assumptions related to the setup of the problem.
Doc Al said:Do your own work, show what you did and where you got stuck, and then you'll get plenty of help.
Doc Al said:You are dealing with point charges here: Look up expressions for the electric field and electric potential at a given distance from a point charge. Note that electric field is a vector, but potential is a scalar.
Electric field is a vector, so direction counts. Add them like vectors.chrisych said:E = Q / (4 pi eo r^2)
For +Q, E1 = Q / (4 pi eo 4^2) = Q / (64 pi eo)
For -Q, E2 = -Q / (4 pi eo 4^2) = -Q / (64 pi eo)
E1 + E2 = ?
Good!V = Q / (4 pi eo r)
For +Q, V1 = Q / (4 pi eo 4) = Q / (16 pi eo)
For -Q, V2 = -Q / (4 pi eo 4) = -Q / (16 pi eo)
V1 + V2 = 0 and so this is the correct answer?
That would be true if E1 and E2 were perpendicular, but they are not. Consider the horizontal & vertical components of each.chrisych said:|E| = sqrt (E1^2 + E2^2)
Doc Al said:That would be true if E1 and E2 were perpendicular, but they are not. Consider the horizontal & vertical components of each.
Typo here; this should be:chrisych said:|E| = |Horizontal Component of E| + |Vertical Component of E|
Doc Al said:You got it!
Typo here; this should be:
|E|^2 = |Horizontal Component of E|^2 + |Vertical Component of E|^2