Save
Physics B
Save
Share
Learn
Content
Leaderboard
Learn
Created by
Christian Policar
Visit profile
Cards (24)
Electric
Circuit
an interconnection of electrical elements that provides a
closed-loop
path for the flow of
electrons
Open, Closed, and Short
Types of
Electric Circuits
Active
and
Passive
Circuit Elements
Active Elements
are sources of electrical energy
Ex.
Voltage
and
Current
source
Passive Elements
are elements that use or dissipate electrical energy
Ex.
Resistor
, Inductor,
Capacitor
, and Memristor
Voltage
is directly
proportional
to the current
Resistance
the electrical property of a material to
oppose
or
limit
the passage of current through it
is the measure of how much a
conductor
resists the flow of
charges
Conductance
,
G
the
reciprocal
of resistance
Current
is the
rate
at which
charge
flows through an area
I = Q/t = dQ/dt
Electron flow
actual
direction of current
charges flow from
negative
terminal to
positive
terminal of the voltage source
Conventional flow
direction used in
circuit analysis
charges flow from
positive
to
negative
terminal of the voltage source
Current Density
current per unit area
J = I/A
in Ampere / m^2
directly proportional to the Electric Field Strength in the conductor
J = I/A = σE
where σ =
conductivity
or specific
conductance
of a material
Resistivity
is the
ratio of the electric field and current density
ρ = E/J
where:
ρ in V/m
E in V/m
J in A/m^2
greater
the ______ the length and resistivity and the smaller the cross-sectional area, the _______ the resistance
R = ρL/A
Temperature effects on resistance
Conductors:
increased temperature =
increased
resistance. conductors have a
positive
temperature coefficient.
Semiconductors:
increased temperature =
decreased
resistance. semiconductors have a
negative
temperature coefficient.
Insulators:
same with
semiconductors.
negative
temperature coefficient.
Electromotive forces
produces a
steady flow of charges
to maintain a potential difference between a pair of terminals
amount of energy provided
by the device to the charges passing through it
supplies energy
and
does NOT apply force
Charge pump
the source moves charges
uphill from the lower potential to the higher
internal resistance
resistance inside
the source of EMF which
cannot be removed
Terminal Voltage
potential difference
between two terminals of a practical source of EMF
When
no current exists
,
VT is equal to the EMF of the battery
VT = ε
Case 1
of Terminal Voltage
When
supplying or delivering power (discharging,)
VT is equal to the EMF - the Voltage drop in the total internal resistance
VT = ε - Ir
Case 2
of
Terminal Voltage
When
receiving power (charging)
, VT is equal to EMF plus the voltage drop in the total internal resistance
VT = ε + Ir
Case 3
of Terminal Voltage
PL = I^2 x R
can also be expressed as
PL = εI - I^2 x r
Current
comes out of
its positive terminal
Power delivered to the load
PL = VT x I
can also be expressed as:
PL = εI + I^2 x r
Current
enters
its positive terminal
Power received by the source