Abstract
This experiment was performed with the purpose of finding and plotting the electric field vector components
across a two-dimensional surface. The electric potential data was obtained for every corresponding (x,y) point
and converted into a list by using the (DAQ). The surfaces tested wi...
Lab 2 Electric Potential & Electric Fields
Abstract
This experiment was performed with the purpose of finding and plotting the electric field vector components
across a two-dimensional surface. The electric potential data was obtained for every corresponding (x,y) point
and converted into a list by using the (DAQ). The surfaces tested with the measuring probe consisted of four
uniform shapes which include the following: Dipole, point plate, sphere, sharp point, and additional diamond
custom shaped surface. Additionally, the voltage probe attributed high electrical potential differences from the
points in the surface with respect to the ground and assigned the color red. Lower potential differences were
assigned the blue color and a “thermo” map was able to be generated from these program specifications.
1. Introduction of the electric field
with respect to r, the
The electric distance traveled.
potential is defined as Electric field always
the absolute travels away from
summation of the positive charges and
electric field from two towards negative
defined bounds. In charges. In the same
other words, at a way, the field moves
certain location on a from a higher potential
surface, the electric to a lower potential. It
potential is obtained is similar to
by taking the integral gravitational field in
of the electric field this way.
from the ground
coordinate to such
point of interest on
such surface. This is a
location dependent
variable that expresses
the amount of
potential energy per When a current
unit of charge at a runs through a
specific spot. The conductor, the charge
difference in potential across the whole
between two points is surface is equalized
called voltage. For a because the electrons
moving charge, the move freely to where
potential difference is they are equidistant
the change in potential from each other. This
between its initial results in the potential
position and its final being equal across the
position. The potential shape of the
difference is also equal conducting surface.
to the negative integral
1
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