Sci I - Symmetry and Gauss’s Law

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33 Terms

1
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How does symmetry simplify modeling forces in physics?

By showing that components of forces in opposite directions can cancel out.

2
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What is an example of symmetry with tugboats?

If two tugboats pull a ship in exactly opposite directions with the same strength, the net force is zero.

3
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What happens if tugboats pull mostly forward but partially opposite?

The forward components add, the left/right components cancel, and the ship moves forward.

4
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How does symmetry apply to two positive charges with a proton in between?

The proton is repelled equally by both charges, so net force is zero.

5
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What does it mean for the electric field at the midpoint between two equal positive charges?

The net electric field is zero at that point.

6
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If the proton is nudged slightly forward between two charges, what happens?

Forward components of the electric fields add, and the proton moves forward.

7
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How do the horizontal components of the fields behave in this scenario?

They cancel out due to symmetry.

8
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How do the vertical components of the fields behave when the proton moves slightly forward?

They point in the same direction and add together.

9
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Why is symmetry useful in electric field calculations?

It allows us to ignore components that cancel out, simplifying the model.

10
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What happens to a proton above a large, flat sheet of positive charge?

It is pushed upward by charges directly below and diagonally upward by charges off to the side.

11
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How does symmetry affect the left/right components of the electric field from a sheet of charge?

They cancel out, leaving only the upward component.

12
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What is the direction of the electric field from a flat sheet of charge?

Straight lines perpendicular to the sheet.

13
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How do electric fields behave between two oppositely charged plates?

They reinforce each other, creating a uniform field.

14
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What technique allows us to find the electric field for extended objects?

Gauss’s law.

15
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What is Gauss’s law equation?

ϕE = q / εo

16
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What does εo represent in Gauss’s law?

The permittivity of free space, a constant.

17
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How is εo related to the Coulomb constant k?

εo = 1 / (4πk)

18
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What does q represent in Gauss’s law?

The total charge contained within the Gaussian surface.

19
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What is electric field flux (ϕE)?

A scalar quantity representing the amount of electric field passing through a given area.

20
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How is electric field flux calculated for a uniform field?

E multiplied by the surface area A.

21
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Give a real-world analogy for flux using rain and a bucket.

Holding a bucket upright captures more rain flux; sideways captures none; angled captures partial flux.

22
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What happens to flux if the bucket has no bottom?

Positive flux enters through the top, negative exits through the bottom; total flux is zero.

23
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What is a Gaussian surface?

An imagined closed geometric shape surrounding an object to calculate electric flux.

24
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Which shape is used for a flat sheet of charge?

A cylinder.

25
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Why does no flux pass through the sides of the Gaussian cylinder?

The sides are parallel to the electric field.

26
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How do we calculate flux through the top and bottom of the cylinder?

Each has area A, and the flux is E*A for each.

27
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What is the flux equation for a cylinder above a sheet of charge?

2 * E * A = q / εo

28
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What is surface charge density σ?

The amount of charge per unit area on the sheet.

29
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How do we express total charge in terms of σ?

q = σ * A

30
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How do we solve for the electric field from a sheet of charge?

E = σ / (2 * εo)

31
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Does the electric field from a sheet of charge depend on position?

No, it is constant everywhere above the sheet.

32
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How does the field from a sheet differ from that of a point charge?

It is constant, not an inverse square law.

33
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Why is using electric fields advantageous over calculating every particle-to-particle force?

Because we calculate the field once, instead of computing interactions between all individual charges.

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