Electric Potential Energy and Work

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Flashcards covering concepts related to electric potential energy, work, and equipotential surfaces.

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12 Terms

1
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Electric Force on Proton vs. Electron

In a constant electric field, a proton and an electron experience the same magnitude of electric force, but in opposite directions due to their opposite charges.

2
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Acceleration of Proton vs. Electron

In a constant electric field, an electron has a larger acceleration than a proton because the electron is much less massive.

3
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Kinetic Energy of Proton vs. Electron

In a constant electric field, a proton and an electron acquire the same kinetic energy when striking the opposite plate because they have the same initial electric potential energy and energy is conserved.

4
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Work and Potential Energy

The work needed to assemble a collection of charges is the same as the total potential energy (PE) of those charges. PE is added over all pairs.

5
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Electric Potential

The total potential is equal to V1 + V2, the total potential is positive.

6
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Electric Potential at Equidistant Points

If two equal and opposite charges are equidistant from a point, the total electric potential at that point is zero.

7
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Electric Field (E) and Potential (V) at the Center of a Square

With +Q and -Q charges at the corners, the electric potential (V) is zero because scalar contributions cancel, but the electric field (E) is non-zero because vector contributions add up.

8
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Equipotential Surfaces

Points equidistant from equal and opposite charges have a potential of V=0. The electric field is not zero at these points.

9
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V = 0 on the x-axis

V = 0 when opposite charges lie directly across the x axis from each other, the potentials from the two charges above the x axis cancel the ones below the x axis.

10
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V = 0 on the y-axis

V = 0 when opposite charges lie directly across the y axis from each other, the potentials from the two charges above the y axis cancel the ones below the y axis.

11
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Points with the Same Potential

Points that are at the same distance from a charge Q are at the same potential and lie on an equipotential surface.

12
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Work and Electric Potential

Moving a positive charge against the electric field requires the most work. Easiest when the field does all the work. Moving along an equipotential requires no work.