announcements exams will be returned tomorrow! homework for tomorrow… ch. 29: cq 1, probs. 4...

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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 pm R 8-12 pm, 2-6 pm T 8-1 pm, 2-6 pm F 8-10 am, 2-5 pm

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Page 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

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 pm R 8-12 pm, 2-6 pm T 8-1 pm, 2-6 pm F 8-10 am, 2-5 pm

Page 2: 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

Chapter 29

Potential & Field(Connecting Potential and Field &

Sources of Electric Potential)

Page 3: 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

29.1: Connecting Potential & Field

Force concepts

Energy concepts

Page 4: 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

29.1: Connecting Potential & Field

Force concepts

Energy concepts

Page 5: 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

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

Page 6: 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

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 si & sf

29.1: Connecting Potential & Field

Page 7: 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

Ex. 29.1:Finding the Potential

The figure below is a graph of Ex, the x-component of the electric field, versus position along the x-axis.

Find and graph V(x). Choose V = 0V at x = 0m.

Page 8: 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

Ex. 29.1:Finding the Potential

The figure below is a graph of Ex, the x-component of the electric field, versus position along the x-axis.

Find and graph V(x). Choose V = 0V at x = 0m.

Page 9: 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

Quiz Question 1This 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. 2000V2. 1000V3. 0V4. -1000V5. -2000V

Page 10: 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

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

Page 11: 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

Ex. 29.2:The potential of a parallel-plate capacitor

Find the electric potential inside the capacitor. Let V=0V at the negative plate.

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