Chapter 5 Electrostatics and Magnetism Flashcards

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1
Q

Electrostatics Definition

A

The study of stationary charges and the forces that are created by and which act upon these charges

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2
Q

Ground definition

A
  • A means of returning charge to the earth

- Ex: doorknob

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3
Q

Static Charge Buildup/Static Electricity-More significant in what environment

A

-More significant in drier air because lower humidity makes it easier for charge to become and remain sparated

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4
Q

SI unit of Charge- Coulomb Value

A

e=1.60 x 10^-19 C

  • protons and electrons both have this amount of charge (while proton +e and electron -e)
  • same magnitude of charge, but not the same mass. Proton much greater mass than electron
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5
Q

Insulator

A

-Will not easily distribute a charge over its surface and will not transfer that charge to another neutral object very well

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6
Q

Conductor

A
  • When a conductor is a given charge, the charges will distribute approx. evenly upon the surface of the conductor
  • Generally metals, but ionic (electrolyte) solutions are also effective conductors
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7
Q

Coulomb’s Law Equation

A
  • Quantifies the magnitude of the electrostatic force Fe between two charges
  • Fe=kq1q2/r^2
  • Fe=magnitude of the electrostatic force
  • k=Coulomb’s constant
  • q1&q2=the magnitudes of the two charges
  • r=distance between the charges
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8
Q

Coulomb’s Constant

A
  • Dependent on the units used in the equation

- SI units k=1/4piEo=8.99x10^9 n*m^2/C^2 where Eo(sigma naught) represents the permittivity of free space

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9
Q

A positive charge is attracted to a negative charge a certain distance away. The charges are then moved so that they are separated by twice the distance. How has the force of attraction changed between them?

A

(Based on Coulomb’s Law) The force between two charges varies as the inverse of the square of the distance between them. So if the distance is double, the square of the distance is quadrupled, so the force is reduced to one-fourth of what is was originally.

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10
Q

Magnitude of an electric field equation

A

E=fe/q=kQ/r^2

  • Fe= magnitude of the force felt by the test charge q
  • k=electrostatic constant
  • Q=the source charge magnitude
  • r=distance of the two charges
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11
Q

Fe/q use:

A
  • place test charge q at some point in electric field, measure the force exerted on that test charge, and define the electric field at that point in space as the ratio of the force magnitude to test charge magnitude
  • *** test charge must actually be present in order for a force to be generated and measured
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12
Q

kQ/r^2

A
  • Does not require the presence of a test charge
  • Only need to know the magnitude of the source charge and the distance between the source charge and point in space where you want to measure the electric field
  • Need to know the value of the source charge to be able to calculate the electric field
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13
Q

Electrical Potential Energy

A

-Form of potential energy that is dependent on the relative position of one charge with respect to another charge or to a collection of charges

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14
Q

Electrical Potential Energy Equation

A

U=kQq/r
-if the charges are like charges (both positive or both negative), the potential energy will be positive. If the charges are unlike (one positive and the other negative) the potential energy will be negative

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15
Q

Electrical Potential

A

The ratio of the magnitude of a charge’s electrical potential energy to the magnitude of the charge itself

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16
Q

Electrical Potential Equation

A

V=U/q

  • V=electrical potential measured in volts (V) & 1V=1J/C
  • If there is no test charge q, you can still calculate the electrical potential of a point in space in an electric field as long as you know the magnitude of the source charge and the distance from the source charge to the point in space in the field– V=kQ/r
  • For a positive source charge, V is positive. For a negative source charge, V is negative
17
Q

Voltage

A

The potential difference between points Va and Vb

Vb-Va

18
Q

Change in Voltage

A

ΔV=Vb-Va=Wab/q

  • Wab is the work needed to move a test charge q through an electric field from point a to point b
  • Work is independent of the actual pathway taken and only depends on the potentials at the two points a and b
19
Q

Equipotential line

A

A line on which the potential at every point is the same

-potential difference between points = 0

20
Q

Electric dipole

A
  • results from two equal & opposite charges being separated by a small distance d from eachother
  • can be transient (like moment by moment changing distribution of elections in the electron cloud of an atom)
  • can be permanent (like molecular dipole of water or the carbonyl functional group)
21
Q

Diamagnetic materials

A

-Made of atoms with no unpaired electrons and that have no net magnetic field

22
Q

Paramagnetic materials

A
  • Become weakly magnetized in the presence of an external magnetic field, aligning the magnetic dipoles with the external field
  • Upon removal of the external field, the thermal energy of the individual atoms will cause the individual magnetic dipoles to reorient randomly
23
Q

Ferromagnetic materials

A
  • have unpaired electrons and permanent atomic magnetic dipoles that are normally oriented randomly so the material has no net magnetic dipole.
  • Different from paramagnetic materials bcs ferromagnetic become strongly magnetized when exposed to a magnetic field or under certain temperatures
  • Bar magnets are ferromagnetic materials with a north and south pole. Field lines exit the north pole and enter the south pole.
24
Q

Lorentz Force

A

The sum of electrostatic and magnetic forces acting on a charge at the same time