Electric circuits Flashcards
Ohmic conductor
and obvious opposites of non-ohmic conductors
Conductor with resistance that is constant for a wide range of :
-voltages
-currents
and obeys ohms law
Voltage
and unit analysis
Difference in electric potential energy per unit charge measured across two points
V = J.C-1
V=W/Q
Current
Measure of electric charge passing through a conducting material/point per unit time
A = J.C-1
I = Q/t
Emf
Electric potential difference between terminals of a battery when NO current is flowing.
OR
Energy per unit charge needed to move an electron from + to - terminal of the battery
V= J.C-1
Resistance
obstacle to the flow of charge
- Ration of voltage over current strength
1 ohm = 1 V.A-1
Ohm’s law
The potential difference across a conductor is directly proportional to the current in the conductor at constant temperature.
Power
The rat eat which work is doen ( P = W/t)
The rate at which electrical energy is transformed /converted into other forms of energy
W = J.s-1
Voltage and current in series and parallel circuits
Series: Current =, voltage /
Parallel: Current /. voltage =
Note on energy given per electron through the circuit in relation to resistors’ effects
Every Coulomb that goes through the circuit loses the same # energy.
Different resistors limit the amount of coulombs NOT THE ENERGY PER COULOMB (thus resistor affect current not voltage as V = W/Q)
Internal resistance
The resistance inside a cell due to the loss of electric potential energy per coulomb as charge leaves/enters the cell
4 factors affecting r
- Size of cell
- Chemical properties
- Age
- Temperature
- Current of the battery
Terminal potential difference (Vload)
Potential difference across the terminals of a battery when there IS A CURRENT flowing in the circuit
Vload = IRext
Lost Volts
The difference between the emf and the terminal potential difference
Emf = Vint + Vload
Vint + Vext
Short circuit and 2 consequences
A path of very low resistance
What happens?
R tends to zero and I tends towards Imax
Consequences:
- The wire heats up rapidly
- the cell goes flat very quickly
Faraday’s Law
The magnitude of the emf induced in a coil is proportional to the rate of change of magnetic flux
Emf = -N Phi/delta t