Lecture 5.1 : Electric Potential Continued · Two protons, one after the other, are launched from...

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1 Lecture 5.1 : Electric Potential Continued Lecture Outline: Electric Potential Potential Inside a Parallel-Plate Capacitor Potential of Point Charges Feb. 11, 2013 Textbook Reading: Ch. 28.4 - 28.7

Transcript of Lecture 5.1 : Electric Potential Continued · Two protons, one after the other, are launched from...

Page 1: Lecture 5.1 : Electric Potential Continued · Two protons, one after the other, are launched from point 1 with the same speed. They follow the two trajectories shown. The protons’

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Lecture 5.1 :Electric Potential Continued

Lecture Outline:Electric Potential

Potential Inside a Parallel-Plate CapacitorPotential of Point Charges

Feb. 11, 2013

Textbook Reading:Ch. 28.4 - 28.7

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Announcements

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•HW5 due next Mon. (2/18) at 9pm on Mastering Physics.

•Please fill out the clicker form I e-mailed if you haven’t already.

•Due to special colloquium today, my office hours today will be cut short ( 3:00-3:45pm). Let me know if you would like to meet some other time.

•Exam #1:

‣Average was 55.4% ± 15.0%

‣Curve: Your Curved Score = (Your UnCurved Score)^0.65 * 100^0.35

‣Example: You scored 50%. Curved score = 50^0.65 * 100^0.35 = 63.7%

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Last Lecture...

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Define s=0 at negative plate, and U0 is potential at s=0.

We discussed the potential energy (U) associated with the location of a charge (q) in an external electric field (E).

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Last Lecture...

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A Positive charge increases in potential energy as it approaches the positive side of a capacitor. Since energy is conserved, its kinetic energy must simultaneously decrease.

Analogous to lifting an object above the earth to increase its potential energy.

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Last Lecture...

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We derived the potential energy shared by two point charges by calculating the Work done by one charge on the other.

Looks like Coulomb’s Law, but it’s different!

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Electric Potential

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Alessandro Volta

We introducted “Electric Field” to indicate an electric charge’s alteration of space. Now we

need a concept of potential energy at all points in space due to a source charge.

V ≡ Uq+sources

q

1 volt = 1 V ≡  1 J/C

Electric Potential:

1.5 V Battery

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Electric Potential

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∆U = q∆V

∆V = Potential Difference, or Voltage.

Since Energy is always conserved, a charged object that is gaining Potential Energy must lose the same amount of Kinetic Energy.

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Electric Potential

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What is the speed of a proton that has been accelerated from rest through a potential difference of -1000V?

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Clicker Question #1

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If a positive charge is released from rest, it moves in the direction of

A. Higher electric potential.B. Lower electric potential.C. Need more information.

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Clicker Question #2

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Two protons, one after the other, are launched from point 1 with the same speed. They follow the two trajectories shown. The protons’ speeds at points 2 and 3 are related by

A. v2 > v3.B. v2 = v3.C. v2 < v3.D. Not enough information to compare their speeds.

NOTE: This answer can be seen most easily if you use Energy Conservation arguments. If you use kinematic arguments, be

careful to note that the two trajectories don’t take equal time!

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Potential Inside a Parallel Plate Capacitor

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Potential Inside a Parallel Plate Capacitor

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Equipotential Surfaces are surfaces with the same

value of V at every point.

Where are the equipotentials in this

drawing?

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Potential Inside a Parallel Plate Capacitor

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Batteries are sources of potential differences!

Think of water being pumped up a hill, then flowing back downhill.

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Potential of Point Charges

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3D Map of Potential around a positive charge.

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Clicker #3

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What is the ratio VB/VA of the electric potentials at the two points?

A. 9.B. 3.C. 1/3.D. 1/9.E. Undefined without knowing the charge.

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Potential of Point Charges

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In a semiclassical model of the hydrogen atom, the electron orbits the proton at a distance of 0.053nm. What is the electric potential of the proton at the

position of the electron?

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Potential of Point Charges

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V =�

i

1

4π�0

qiri

3D Map of Potential around dipole.

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Potential of Point Charges

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What is the potential at the point indicated?

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Clicker #4

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At the midpoint between these two equal but opposite charges:

A. E = 0; V = 0.B. E = 0; V > 0.C. E = 0; V < 0.D. E points right; V = 0.E. E points left; V = 0.

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Potential of Point Charges

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Continuous distributions of charge?

Vring on axis =1

4π�0

Q√R2 + z2

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Reminders

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•Stay up to date on your textbook reading. You should finish reading Ch. 28, and start on Ch. 29.

•Begin working on HW5.