announcements exams will be returned tomorrow! homework for tomorrow… ch. 29: cq 1, probs. 4...
TRANSCRIPT
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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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Chapter 29
Potential & Field(Connecting Potential and Field &
Sources of Electric Potential)
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29.1: Connecting Potential & Field
Force concepts
Energy concepts
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29.1: Connecting Potential & Field
Force concepts
Energy concepts
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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
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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
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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.
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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.
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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
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Connecting V & E for a point charge…i.e. Use the E-field of a point charge to find its electric potential..
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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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