AP Physics C: E&M Unit 8 Formulas

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34 Terms

1
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Formula(s) for electric field?

\overrightarrow{E} = \frac{\overrightarrow{F}_e}{q_0} = k_e\frac{q}{r_0²}\hat{r}

2
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What sign is the test charge always assumed to be?

positive

3
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Formula for electric force for point charges only?

\overrightarrow{F}_e = q\overrightarrow{E}

4
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q>0, what direction are the force and field in?

same direction

5
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q<0, what direction are the force and field in?

opposite directions

6
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For a positive particle, how are the field lines oriented?

radially outward

7
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For a negative particle, how are the field lines oriented?

radially inward

8
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Two equal yet oppositely charged particles are at radius r. What are some properties of the field?

  • Field is strongest in the middle of the two charges

  • Lines from + go to infinity

    • Lines to - start at infinity and terminate at the charge

9
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Where do field lines start and terminate?

start at + and terminate at -

10
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Two equal charges with same sign are at a distance r. What are the properties of the field?

  • Field is 0 at the center

  • Lines end infinitely far away

    • Far away, the field is roughly like a charge of 2q

11
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Two unequal and opposite charges are at distance r. What are the properties of the field?

  • x lines leave the greater charge for every y of the opposite charge

    • Far away, the field is roughly that of a single charge

12
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Uniform fields have constant _____?

acceleration

13
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Integral definition for electric fields?

\overrightarrow{E} = k\int \frac{1}{r²}\hat{r}dq

14
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Linear charge density?

\lambda = \frac{q}{L}

15
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Surface charge density?

\sigma = \frac{q}{A}

16
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Volumetric charge density?

\rho = \frac{q}{V}

17
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Electric fields are extremely long distances (linear density)?

\overrightarrow{E}_x = \frac{2k\lambda}{D}

18
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Electric fields for points perpendicular to a line of charge?

\overrightarrow{E}_x = \frac{kQ}{D\sqrt{D²+(\frac{L}{2})²}}

19
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Perpendicular electric fields for full rings of charge at a distance D from the center axis?

0

20
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Parallel electric fields for charged rings at a distance D on the center axis?

\overrightarrow{E} = \frac{kDQ}{(R²+D²)^{\frac{3}{2}}}

21
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Electric fields for arcs of charge?

\overrightarrow{E} = k \cdot \frac{\lambda}{R} \int_{-\alpha}^{\alpha} cos(\theta)d\theta \hat{i}

22
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Gauss’s Law formula?

\Phi_E = \oint \overrightarrow{E} \cdot dA = E \cdot Acos(\phi) = \frac{Q_{enc}}{\epsilon_0}

23
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When is \frac{Q_{enc}}{\epsilon_0} used for Gauss’s law?

Enclosed surfaces

24
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When is the dot product E \cdot Acos(\phi) used for Gauss’s Law?

non-enclosed surfaces

25
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At what angle is flux at its maximum?

when \phi = 0

26
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At what angle is flux at a minimum?

when \phi = 90

27
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Does changing the radius of a gaussian surface change the flux?

no

28
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Does changing the shape of a gaussian surface change the flux?

no

29
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Does changing the location of the interior charge of a gaussian surface change the flux?

no

30
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Does changing the enclosed charge value of a gaussian surface change the flux?

yes

31
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What are some flux/field properties of conductive sheets?

  • The field is 0 inside the material

  • Creates charge density on both sides

32
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What are some flux/field properties of insulating sheets?

  • Field is a non-zero value inside the material

    • Charging makes a charge density on only one side

33
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Field equation for conductive sheets?

\overrightarrow{E} = \frac{\sigma}{\epsilon_0}

34
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Field equation for insulating sheets?

\overrightarrow{E} = \frac{\sigma}{2\epsilon_0}