Difference between revisions of "Chapter 23 Problem 35"

From 105/106 Lecture Notes by OBM
(Created page with "== Problem == thumb|right|The disc with a hole A flat ring of inner radius <math>R_1</math> and outer radius <math>R_2</math> carries a unifo...")
 
 
Line 1: Line 1:
 
== Problem ==
 
== Problem ==
[[File:Chapter23_problem35q.png|thumb|right|The disc with a hole]]
+
[[File:Chapter23_problem35q.png|center|300px|The disc with a hole]]
 
A flat ring of inner radius <math>R_1</math> and outer radius <math>R_2</math> carries a uniform surface charge density <math>\sigma</math>. Determine the electric potential at points along the x axis
 
A flat ring of inner radius <math>R_1</math> and outer radius <math>R_2</math> carries a uniform surface charge density <math>\sigma</math>. Determine the electric potential at points along the x axis
 
== Solution ==
 
== Solution ==
Line 9: Line 9:
 
<math>dq=\sigma dA=\sigma (2\pi R dR)</math>
 
<math>dq=\sigma dA=\sigma (2\pi R dR)</math>
  
<math>V=\frac{1}{4\pi\epsilon_0}\int\frac{dq}{r}=\frac{1}{4\pi\epsilon_0}\int\frac{\sigma (2\pi R dR)}{\sqrt{x^2+R^2}}</math>
+
<math>V=\frac{1}{4\pi\epsilon_0}\int_{R_1}^{R_2}\frac{dq}{r}=\frac{1}{4\pi\epsilon_0}\int_{R_1}^{R_2}\frac{\sigma (2\pi R dR)}{\sqrt{x^2+R^2}}</math>
  
<math>=\frac{\sigma}{2\epsilon_0}\int\frac{R}{\sqrt{x^2+R^2}dR}</math>
+
<math>=\frac{\sigma}{2\epsilon_0}\int_{R_1}^{R_2}\frac{R}{\sqrt{x^2+R^2}}dR</math>
  
 
<math>x^2+R^2=u\rightarrow 2RdR=du\rightarrow RdR=\frac{1}{2}du</math>
 
<math>x^2+R^2=u\rightarrow 2RdR=du\rightarrow RdR=\frac{1}{2}du</math>

Latest revision as of 22:29, 24 February 2020

Problem

The disc with a hole

A flat ring of inner radius and outer radius carries a uniform surface charge density . Determine the electric potential at points along the x axis

Solution

The disc from the chapter

This is just a disc removed from the full disc we already solved in the chapter. Let's recycle things from there.

i.e. you just remove the inner hole's contribution from the total solution