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Kirchhof's current Law
The sum of the magnitudes of the currents directed into a junction equals the sum of the magnitudes of the currents directed out of a junction.
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Ohm's Law
The current through a conductor between two points is directly proportional to the potential difference across the two points. V=IR
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Electric Potential
The electric potential V at given point is the electric potential energy EPE of a small test charge qo situated at that point, divided by the charge itself V=EPE/qo
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The Law of Conservation of Charge
During any process, the net electric charge of an isolated system remains constant
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Electric Field
The electric force, F, per unit charge that is operating on a small test charge qo (+) at that point.
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Electric Field Lines
- Electric charges create an electric field
- Electric Field lines are used to indicate the direction and strength of that field.
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Electric field Lines: The Rules
- - Lines go towards negative charges and away from positive charges
- - Lines radiate into three-dimensional space
- - Lines start at a positive charge and finish at a negative one, i.e. they do not terminate mid-way between charges
- - Lines cannot cross each other
- - When field lines are parallel to each other (i.e. equidistant from each other), this indicates that electric field strength is uniform
- - When electric field lines are close together, this indicates the region where the field strength is greatest
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Electric Dipole
Two point charges with the same magnitude but opposite sign, separated by distance, d.
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The Electron Volt (eV)
- The amount of work W=qo V must be done to move a charge qo through a potential difference, V, 1.6x10-19 C is the charge on the electron, and therefore, to move it through a potential difference of 1V, the amount of work that must be done is W=1.6x10-19 C x 1V = 1.6x10-19 J
- 1eV = 1.6x10-19 J
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Equipotential Surface
- Spherical surfaces which have the same electric potential at every point.
- No work is done be the electric force when a test charge moves along any route on an equipotential surface.
- WABC=0
- Work IS done when a test charge moves BETWEEN equipotential surfaces WAD≠0
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