Current is the flow of charge, measured in ampères, or amps (A).
The Vrms = 6.4 X √2 = 4.5 V.
Charge is measured in coulombs (C), which is defined as: 1 coulomb is the quantity of charge carried past a given point if a steady current of 1 amp flows for 1 second.
1 electron carries a charge of 1.6 ´ 10-19 C.
1 coulomb is equivalent to 6.2 ´1018 electrons.
Charge and current are linked by a simple formula: Charge (C) = current (A) X time (s).
There are some important multipliers for current: 1 microamp (1µA) = 1 X 10 -6 A, 1 milliamp (mA) = 1 X 10 -3 A.
Chemical reactions inside a cell help to create a small POTENTIAL DIFFERENCE between the terminals and this makes the electrons flow along any conducting path that connects them.
A current (flow of charge) will flow through an electrical component (or device) only if there is a voltage or potential difference (p.d.) across its ends.
The bigger the potential difference across a component, the bigger the current that flows through it.
The conducting path through the bulbs, wire and battery is called a circuit.
Ohm’s Law states that the current in a metallic conductor is directly proportional to the potential difference between its ends provided that the temperature and other physical conditions are the same.
An ohmic conductor is a conductor that obeys Ohm’s Law.
Voltage and current can be measured and plotted as a graph called a VI characteristic.
The gradient of a voltage current graph determines the resistance.
A filament lamp’s resistance rises as the filament gets hotter, which is shown by the gradient getting steeper.
A thermistor’s resistance goes down as it gets hotter because the material releases more electrons to be able to conduct.
The diode characteristic graph looks like this: The diode starts to conduct at a voltage of about +0.6 V, which is called forward bias, and then the current rises rapidly for a small rise in voltage.
If the current is reversed (reverse bias), almost no current flows until the breakdown voltage is reached, which usually results in destruction of the diode.
Resistivity is a property of the material and is defined as the resistance of a wire of the material of unit area and unit length.
In a series circuit, the electrons in the current have to pass through all the components, which are arranged in a line.
In a parallel circuit, the current splits into the number of branches there are.
The cell is a source of Chemical potential energy.
The cell does work on electrons and the electrons gain Electrical potential energy (we call it just potential energy).
P.D
(Potential difference or Voltage) across battery terminals indicates the potential energy given to each coulomb (approximately 1018 electrons) of charge.
If 1 Joule of energy is given to 1 Coulomb of electric charge by the battery then we say that the p.d
across the cell is 1 Volt.
When the charges move through the wire they do not lose any of the potential energy they are carrying.
When they pass through something that resists their flow, they will have to do work.
If two or more resistors are connected in parallel, they give a lower resistance than any one of the resistors by itself.
Kirchhoff's Laws: The algebraic sum of currents at a junction is zero, and around a closed circuit loop, the algebraic sum of the e.m.f.s is equal to the algebraic sum of the p.d.s.
Kirchhoff I: The algebraic sum of currents at a junction is zero.
Kirchhoff II: Around a closed circuit loop, the algebraic sum of the e.m.f.s is equal to the algebraic sum of the p.d.s.
Batteries convert chemical energy into electrical energy, and generators turn kinetic energy into electrical energy.
A battery does a job of work in pumping the electrons around the circuit.
Positive charges do not move.
A battery is said to produce Emf (electromotive force) which is defined as the energy converted into electrical energy when unit charge passes through the source.
The energy supplied to a circuit by a battery is given by: W = Q * ε, where W is the energy in J, Q is the charge in C, and ε, curly E is the physics symbol for emf.
No circuit at all is 100 % efficient, some energy is dissipated in the wires, or even in the battery itself.
All batteries and generators dissipate heat internally when giving out a current, due to internal resistance.
A perfect battery has no internal resistance, but unfortunately there is no such thing as a perfect battery.