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voltage
difference in electric potential between the two terminals
capacitator on the circuit
stores charge and electric potential energy
conservation of energy
W = ΔUg
stationary source charges
are repelled by charges q
a hand must push to move q closer to the source charges
hand does work
transferring energy into system of charges
ΔUelec = W
Uelec
electric potential energy
of a charge can be determined by computing how much work it took to move the charge to the position
work
energy transferred into a system by pushing on it
a charged particle’s potential energy is
proportional to its charge
electric potential (V)
potential to create an electric potential energy if charge is placed at the point
tells us how the source charges provide q with potential energy
created by the source charge
exists at every point in space
electric potential energy (J)
U = equal to the amount of work done
interaction energy of a charged particle with the source charge
farther from +, U gets smaller
farther from -, U gets bigger
electric potential
only dependent on distance from source charge
other moving charges don’t matter
that potential is always there in space based on source charges
a positive charge at a lower V
loses energy
a negative charge at a lower V
gains energy
conservation of energy equation
Kf + (Uelec)f = Ki + (Uelec)i
Kf + qVf = Ki + qVi
Kf - Ki = Ui - Uf
ΔK = -ΔU = -qΔV
motion of charges
ΔK = -qΔV
for a positive charge
positive K → speeds up
negative K → slows down
negative charges are the opposite
positive charge
speeds up from high to low potential
slow down from low to high
negative charge
speeds up from low to high potential
slow down from high to low
a positive and negative charge are released from rest in a vacuum and as they move towards each other
a negative potential energy becomes more negative
1 electron volt = 1 eV
a unit of energy
kinetic energy gained by the electron as it accelerates through a potential difference of 1 volt
K = -qΔV = -(-e)(1) = eV
Vo
potential at the surface of a sphere
= Q/4piEoR
potential outside the sphere charged to potential Vo
V = RVo/r
as distance from center increases, the potential decreases
R = radius of sphere
r = distance from center to point
an electric potential is created
separating a positive charge from a negative charge
requires work for the separation
metal wires connecting items
every point has the same electric potential
batteries
can create a fixed potential difference using chemicals
voltmeter
can measure potentials with 2 inputs
electric energy can be
transformed to other types of energy (kinetic, thermal, etc)
when a + charge moves from - to +
potential energy increases
kinetic energy decreases
electric potential inside a parallel-plate capacitor
uniform electric field
Vc = V+ - V- = Ed
equipotential surfaces
the potential of planes is the same throughout the plane
variables of a parallel-plate capacitor
Vc = potential difference between + and -
d = distance between the plates (m)
E = electric field
Q+ = charge on + plate
Q- = charge on - plate
x = distance of the point from the negative plate
V = 0 and x = 0
at the negative plate of a parallel-plate capacitor
V = Vc and x = d
at the positive plate of a parallel-plate capacitor
potential of an electric dipole
sum of potentials of positive and negative charges
in a capacitor, electric field gets stronger and potential differencee increases
as the charge on the electrodes increases
potential difference between electrodes
is proportional to their charge
C
capacitance = constant of proportionality
depends on shape, size, and spacing of electrodes
capacitor
can be charged by a battery
holds the charge even if battery is removed later
a charged capacitor stores energy
as electric potential energy