ch24-p018 - 18. In applying Eq. 24-27, we are assuming V 0...

Info iconThis preview shows page 1. Sign up to view the full content.

View Full Document Right Arrow Icon
18. In applying Eq. 24-27, we are assuming V 0 as r . All corner particles are equidistant from the center, and since their total charge is 2 q 1 – 3 q 1 + 2 q 1 q 1 = 0, then their contribution to Eq. 24-27 vanishes. The net potential is due, then, to the two
Background image of page 1
This is the end of the preview. Sign up to access the rest of the document.

This note was uploaded on 10/28/2010 for the course PHYS 361 taught by Professor Fr during the Fall '10 term at East MS CC.

Ask a homework question - tutors are online