1. Announcements  Exams will be returned TOMORROW!  Homework for tomorrow… Ch. 29: CQ 1, Probs. 4 & 34  Office hours… MW 12:30-1:30 pm TR 9-10 am F 1-2 pm  Tutorial Learning Center (TLC) hours: MW 8-10 am, 12-6 pmR 8-12 pm, 2-6 pm T 8-1 pm, 2-6 pmF 8-10 am, 2-5 pm

2. Chapter 29 Potential & Field (Connecting Potential and Field & Sources of Electric Potential)

3. 29.1: Connecting Potential & Field Force concepts Energy concepts

4. 29.1: Connecting Potential & Field Force concepts Energy concepts

5. 29.1: Connecting Potential & Field  Electric potential and electric field are NOT two distinct entities But rather two different representations of how source charges alter space around them

6.  Electric potential and electric field are NOT two distinct entities But rather two different representations of how source charges alter space around them  Graphically: ΔV = negative of the area under the E vs. s curve between s i & s f 29.1: Connecting Potential & Field

7. Ex. 29.1: Finding the Potential The figure below is a graph of E x, the x-component of the electric field, versus position along the x-axis. Find and graph V(x). Choose V = 0V at x = 0m.

8. Ex. 29.1: Finding the Potential The figure below is a graph of E x, the x-component of the electric field, versus position along the x-axis. Find and graph V(x). Choose V = 0V at x = 0m.

9. Quiz Question 1 This is a graph of the x-component of the electric field along the x-axis. Choose the potential to be zero at the origin. What is the potential at x  1m? 1. 2000V 2. 1000V 3. 0V 4. -1000V 5. -2000V

10. Connecting V & E for a point charge… i.e. Use the E-field of a point charge to find its electric potential..

11. Ex. 29.2: The potential of a parallel-plate capacitor Find the electric potential inside the capacitor. Let V=0V at the negative plate. +++++++++++++++++++++++++++++++ -------------------------------------------------------