History Of Electricity And How Does It Work
Electricity is a
fascinating field where the interplay of physical phenomena associated with
electric charges creates a world of possibilities. As someone with hands-on
experience and a deep-rooted interest in this domain, I've dedicated
significant time and effort to understanding its intricacies.
My
career has spanned various industries, including manufacturing,
pharmaceuticals, and oil and gas, where I've honed my electrical
troubleshooting skills. Roles such as Service Engineer for power press
machinery and Instrument Technician in the oil and gas sector have equipped me
with a comprehensive understanding of electrical systems. While these
experiences were invaluable, the repetitive nature of such roles can be
stifling. I thrive on challenges and find fulfilment in devising innovative
solutions to complex electrical problems.
Beyond
the technical realm, I've ventured into acting, demonstrating my adaptability
and willingness to explore diverse fields. This unconventional path has
enriched my problem-solving approach, making me versatile.
Let's
delve deeper into the captivating world of ELECTRICITY.
Electricity
is related to magnetism, both being part of the phenomenon
of electromagnetism, as described by Maxwell's equations.
Common phenomena are related to electricity,
including lightning, static electricity, electric
heating, electric discharges, etc.
The
presence of either a positive (+) or negative
(-) electric charge produces an electric field. The motion
of electric charges is an electric current and produces
a magnetic field. In most applications, Coulomb's law determines
the force acting on an electric charge. Electric
potential is the work done to move an electric charge from one
point to another within an electric field, typically measured in volts.
Electricity
plays a central role in many modern technologies, serving in electric
power where electric current is used to energise equipment, and
in electronics dealing with electrical
circuits involving active components such as vacuum tubes, transistors, diodes and integrated
circuits, and associated passive interconnection technologies.
The
study of electrical phenomena dates back to antiquity, with theoretical
understanding progressing slowly until, the 17th and 18th centuries. The development
of the theory of electromagnetism in the 19th century marked significant
progress, leading to electricity's industrial and residential application
by electrical engineers by the century's end. This rapid expansion in
electrical technology at the time was the driving force behind the Second
Industrial Revolution, with electricity's versatility driving
transformations in both industry and society. Electricity is integral to
applications
spanning transport, heating, lighting, communications,
and computation, making it the foundation of modern industrial society.
Maxwell's Equations: The Heart of Electromagnetism
Maxwell's
equations are
a set of 4 fundamental equations that describe the behaviour of electric and
magnetic fields. These equations are the cornerstone of classical
electromagnetism, providing a mathematical framework to understand phenomena
ranging from electric circuits to light and radio waves.
The
Four Equations:
While
the complete mathematical representation involves complex calculus, we can
break down the core concepts of each equation:
- Gauss's
Law for Electricity: This equation relates electric charge to
the electric field it produces. Essentially, it states that electric
field lines originate from positive charges and terminate at negative
charges.
- Gauss's
Law for Magnetism: This equation indicates that magnetic field
lines always form closed loops, meaning there are no isolated magnetic
poles (like magnetic monopoles).
- Faraday's
Law of Induction: This law describes how a changing magnetic field
induces an electric field. It's the principle behind electromagnetic
induction, the basis for generators and transformers.
- Ampère's
Law with Maxwell's Addition: This equation relates electric
currents and changing electric fields to the magnetic field they
produce. Maxwell's addition to Ampère's law was crucial, introducing
the concept of displacement current, which is essential for understanding
electromagnetic waves.
Historically,
the finding of electricity is a collaboration of scientists'
finding throughout millennia:
Long
before any knowledge of electricity existed, people were aware of shocks
from electric fish. Ancient Egyptian texts dating from 2750
BCE described them as the "protectors" of all other fish.
Electric fish were again reported millennia later by ancient
Greek, Roman and Arabic naturalists and physicians.
Several ancient writers, such as Pliny the Elder and Scribonius
Largus, attested to the numbing effect of electric shocks delivered
by electric catfish and electric rays and knew that such shocks
could travel along conducting objects. Patients with ailments such
as gout or headache were directed to touch electric fish in
the hope that the powerful jolt might cure them.
Ancient
cultures around the Mediterranean knew that certain objects, such as
rods of amber, could be rubbed with a cat's fur to attract light objects
like feathers. Thales of Miletus made a series of observations
on static electricity around 600 BCE, from which he believed that
friction rendered amber magnetic, in contrast to minerals such
as magnetite, which needed no rubbing. Thales was incorrect in believing
the attraction was due to a magnetic effect, but later science would prove a
link between magnetism and electricity. According to a controversial theory,
the Parthians may have had knowledge of electroplating, based on
the 1936 discovery of the Baghdad Battery, which resembles a galvanic
cell, though it is uncertain whether the artefact was electrical in nature.
Electricity would remain little more than an intellectual curiosity for
millennia until 1600, when the English scientist William
Gilbert wrote De Magnete, in which he made a careful study of
electricity and magnetism, distinguishing the lodestone effect from
static electricity produced by rubbing amber. He coined
the Neo-Latin word electricus ("of amber" or
"like amber", from ἤλεκτρον, Elektron, the Greek word
for "amber") to refer to the property of attracting small objects
after being rubbed. This association gave rise to the English words
"electric" and "electricity", which made their first
appearance in print in Thomas Browne's Pseudodoxia Epidemica of
1646.
Later
in the 18th century, Benjamin Franklin conducted extensive
research in electricity, selling his possessions to fund his work. In June 1752
he is reputed to have attached a metal key to the bottom of a dampened kite
string and flown the kite in a storm-threatened sky. A succession of
sparks jumping from the key to the back of his hand showed
that lightning was indeed electrical in nature. He also explained the
apparently paradoxical behaviour of the Leyden jar as a device for
storing large amounts of electrical charge in terms of electricity consisting
of both positive and negative charges. In 1775, Hugh Williamson reported a
series of experiments to the Royal Society on the shocks delivered by
the electric eel; that same year the surgeon and anatomist John Hunter described
the structure of the fish's electric organs. In 1791, Luigi
Galvani published his discovery of bioelectromagnetics, demonstrating
that electricity was the medium by which neurons passed signals to
the muscles.
Alessandro
Volta's battery, or voltaic pile, of 1800, made from alternating
layers of zinc and copper, provided scientists with a more reliable source of
electrical energy than the electrostatic machines previously used.
The recognition of electromagnetism, the unity of electric and magnetic
phenomena, is due to Hans Christian Ørsted and André-Marie
Ampère in 1819–1820.
Michael
Faraday invented
the electric motor in 1821, and Georg Ohm mathematically
analysed the electrical circuit in 1827. Electricity and magnetism (and light)
were definitively linked by James Clerk Maxwell, in particular
in his "On Physical Lines of Force" in 1861 and 1862.
While
the early 19th century had seen rapid progress in electrical science, the late
19th century would see the greatest progress in electrical engineering.
Through such people as Alexander Graham Bell, Ottó
Bláthy, Thomas Edison, Galileo Ferraris, Oliver
Heaviside, Ányos Jedlik, William Thomson, 1st Baron
Kelvin, Charles Algernon Parsons, Werner von Siemens, Joseph
Swan, Reginald Fessenden, Nikola Tesla and George
Westinghouse, electricity turned from a scientific curiosity into an essential
tool for modern life.
In
1887, Heinrich Hertz: discovered that electrodes illuminated
with ultraviolet light create electric sparks more easily. In
1905, Albert Einstein published a paper that explained
experimental data from the photoelectric effect as being the result
of light energy being carried in discrete quantized packets, energising
electrons. This discovery led to the quantum revolution. Einstein was
awarded the Nobel Prize in Physics in 1921 for "his
discovery of the law of the photoelectric effect". The
photoelectric effect is also employed in photocells such as can be
found in solar panels.
The
first solid-state device was the "cat's-whisker detector"
first used in the 1900s in radio receivers. A whisker-like wire is placed
lightly in contact with a solid crystal (such as a germanium crystal)
to detect a radio signal by the contact junction effect. In a
solid-state component, the current is confined to solid elements and
compounds engineered specifically to switch and amplify it. Current flow can be
understood in two forms: as negatively charged electrons, and
as positively charged electron deficiencies called holes.
These charges and holes are understood in terms of quantum physics.
The building material is most often a crystalline semiconductor.
Solid-state
electronics came into its own with the emergence
of transistor technology. The first working transistor,
a germanium-based point-contact transistor, was invented by John
Bardeen and Walter Houser Brattain at Bell Labs in
1947, followed by the bipolar junction transistor in 1948.
Electricity at the particle level is the Flow of Electrons
Electricity is a form of
energy resulting from the movement of charged particles, primarily
electrons. It's a fundamental force of nature, powering everything from
simple light bulbs to complex electronic devices.
Electron Is A Subatomic Particle
With
a negative charge. It
is one of the fundamental building blocks of matter, along with protons and
neutrons. Electrons orbit the nucleus of an atom, which is composed of protons
and neutrons.
These
electrons act differently in their behaviour in different materials
(characteristic)
his is a fundamental property of the particle. The charge of a single electron is approx = -1.602 x 10^-19 coulombs.
Electrons Are Building Blocks of the Current
As
we've established, electrons are subatomic particles with a negative
charge. They are the fundamental particles responsible for electric
current.
Electric
Current Are The Flow of Electrons
Electric
current is
the rate of flow of electric charge. Essentially, it's the movement
of electrons through a conductor.
- The direction of flow: While
electrons physically move from the negative to the positive terminal of a
battery, conventionally, current is considered to flow from positive to
negative. This is a historical convention that doesn't affect circuit
analysis.
- Measurement: Electric
current is measured in amperes (A). One ampere is equal to one
coulomb of charge passing a point in one second.
Factors That Affects Current:
- Voltage: The
potential difference between two points in a circuit, measured in volts
(V), drives the flow of electrons. A higher voltage results in a
higher current.
- Resistance: The
opposition to the flow of electric current in a material, measured in ohms
(Ω). Higher resistance reduces current flow.
Ohm's
Law relates
these quantities:
- Voltage
(V) = Current (A) * Resistance (Ω)
The
man behind Ohm Law:
Georg
Simon Ohm was
a German physicist who is credited with formulating Ohm's Law. Through
meticulous experimentation, Ohm discovered a fundamental relationship between
voltage, current, and resistance in an electrical circuit.
Ohm's law states that the electric current through a conductor between two points is directly proportional to the voltage across the two points. Introducing the constant of proportionality, the resistance, one arrives at the three mathematical equations used to describe this relationship:
Where I is the current through the
conductor, V is the voltage measured across the conductor
and R is the resistance of the conductor. More
specifically, Ohm's law states that the R in this relation is constant,
independent of the current. If the resistance is not constant, the
previous equation cannot be called Ohm's law, but it can still be used as
a definition of static/DC resistance. Ohm's law is an empirical
relation which accurately describes the conductivity of the vast majority
of electrically conductive materials over many orders of magnitude of
current.
Resistive
circuits
Resistors are
circuit elements that impede the passage of electric charge in
agreement with Ohm's law and are designed to have a specific resistance
value R. In schematic diagrams, a resistor is shown as a long rectangle or
zig-zag symbol. An element (resistor or conductor) that behaves according to
Ohm's law over some operating range is referred to as an ohmic
device (or an ohmic resistor) because Ohm's law and a single value
for the resistance suffice to describe the behaviour of the device over that
range.
Ohm's
law holds for circuits containing only resistive elements (no capacitances or
inductances) for all forms of driving voltage or current, regardless of whether
the driving voltage or current is constant (DC) or time-varying such
as AC. At any instant of time, Ohm's law is valid for such circuits.
Resistors
which are in series or in parallel may be grouped together
into a single "equivalent resistance" to apply Ohm's law in
analyzing the circuit.
Electrical Unit Conversions
Before
diving into conversions, let's review the fundamental electrical units:
- Voltage
(V): Measures
the potential difference between two points in an electrical circuit.
- Current
(A): Measures
the rate of flow of electric charge.
- Resistance
(Ω): Measures
the opposition to the flow of electric current.
- Power
(W): Measures
the rate at which energy is transferred.
- Energy
(Wh or kWh): Measures
the total amount of energy consumed.
Common Conversions
Electrical
unit conversions and their formulas:
Power (W)
- Watts
to Kilowatts (kW): 1 kW = 1000 W
- Watts
to Horsepower (hp): 1 hp ≈ 746 W
Energy (Wh or kWh)
- Watt-hours
to Kilowatt-hours (kWh): 1 kWh = 1000 Wh
- Kilowatt-hours
to Joules (J): 1
kWh = 3.6 x 10^6 J
Current (A)
- Amperes
to Milliamperes (mA): 1 A = 1000 mA
- Amperes
to Kiloamperes (kA): 1 kA = 1000 A
Useful Conversion Formulas
- Ohm's
Law: V
= IR (Voltage = Current * Resistance)
- Power
Law: P
= VI (Power = Voltage * Current)
- Energy: E = Pt (Energy = Power * Time)
Fundamental Laws of Electricity
Electrical
laws are
the foundational principles governing the behaviour of electric charges and
currents. They provide the framework for understanding and analyzing
electrical circuits.
The
Key of Electrical Laws:
- Ohm's
Law: Relates
voltage, current, and resistance in a circuit (V = IR).
- Kirchhoff's
Laws:
- Kirchhoff's
Current Law (KCL): The total current flowing into a junction is
equal to the total current flowing out of it.
- Kirchhoff's
Voltage Law (KVL): The sum of all voltages around a closed loop in
a circuit is equal to zero.
- Joule's
Law: Relates
the heat generated by an electrical current to the resistance, current,
and time.
Coulomb's Law: Describes the force between two electric charges.
- Faraday's
Law of Induction: Explains electromagnetic induction.
- Lenz's
Law: Determines
the direction of induced current.
- Maxwell's
Equations: A
comprehensive set of equations describing electric and magnetic
fields.
There
are two types of Current:
Direct Current (DC)
- Constant
flow: Electrons
move in a single direction.
- Sources: Batteries,
solar cells, and DC power supplies.
- Applications: Electronic
devices, rechargeable batteries, and control systems.
Alternating Current (AC)
- Reversing
flow: Electrons
change direction periodically.
- Sources: Power
plants, electrical grids.
- Applications: Powering
homes, businesses, and industries.
Role Of Rectifier:
AC
to DC conversion is
essential for powering electronic devices that require a steady, unidirectional
current. This process is achieved primarily through the use of rectifiers.
AC Waveforms:
While
we've established that AC power typically follows a sinusoidal waveform, it's
essential to grasp other key characteristics:
- Peak
Voltage (Vp): The
maximum voltage value reached during a cycle.
- Peak-to-Peak
Voltage (Vpp): The
difference between the maximum positive and negative peaks.
- Root
Mean Square (RMS) Voltage (Vr): The equivalent DC voltage that
produces the same heating effect. This is the value typically used for
power calculations.
- Frequency: The number
of cycles per second, measured in Hertz (Hz).
AC Power Calculations
Using RMS values, we can apply Ohm's law and
power formulas similar to DC calculations:
- Power
(P) = Vrms * Irms
- Current
(Irms) = Vrms / R
AC Power Transmission
and Distribution
DC Waveforms
Unlike
AC waveforms, which oscillate over time, DC waveforms are characterized by
their constancy.
An ideal DC waveform is a straight, horizontal line. It represents a constant voltage or current value over time. There are no fluctuations or changes in direction.
Real-world DC Waveforms
In
practical applications, perfect DC waveforms are difficult to achieve. There
are often minor variations due to factors like:
- Ripple: Small
fluctuations caused by the charging and discharging of capacitors in power
supplies.
- Noise: Random
fluctuations due to external interference.
- Load variations: Changes in the current draw can affect the voltage level.
DC
waveform with ripple
Importance of DC Waveforms
Understanding
DC waveforms is essential for:
- Power
supply design: Ensuring
stable and clean DC power for electronic devices.
- Circuit
analysis: Identifying
and mitigating noise or ripple in DC signals.
- Battery performance: Evaluating battery charging and discharging characteristics.
AC to DC Rectification
A
rectifier is an electronic device that converts alternating current (AC), which
periodically reverses direction, to direct current (DC), which flows in
only one direction.
How it works:
- Diodes: The core
components of a rectifier are diodes, which allow current to flow in only
one direction.
- Half-wave rectifier: Uses a single diode to convert one half-cycle of the AC waveform into DC. Full-wave rectifier: Employs four diodes to convert both halves of the AC waveform into DC, providing a smoother output.
Rectification Process
- AC
input: The
AC voltage is applied to the rectifier circuit.
- Diode
conduction: During
the positive half-cycle of the AC input, one or two diodes conduct,
allowing current to flow through the load.
- DC
output: The
output voltage is a pulsating DC, with a ripple component.
Filtering:
To
reduce the ripple in the output, a filter is often used. Capacitors are
commonly employed for this purpose. The capacitor charges during the peak
of the rectified waveform and discharges during the valleys, smoothing out
the output.
Types of Rectifiers
- Half-wave
rectifier: Simpler
but less efficient, with higher ripple.
- Full-wave
rectifier: More
efficient, with lower ripple.
- Bridge rectifier: A common type of full-wave rectifier using four diodes.
AC
to DC conversion is essential in applications:
- Power
supplies for electronic devices
- Battery
chargers
- Inverters
(DC to AC conversion
Characteristics of Diode
The following are the characteristics of the diode:
- Forward-biased diode
- Reverse-biased diode
- Zero biased diode
Forward-biased Diode
There is a small drop of voltage across the diode when the diode is forward-biased and the current is conducting. For silicon diodes, the forward voltage is 690mV and for germanium, 300mV is the forward voltage. The potential energy across the p-type material is positive and across the n-type material, the potential energy is negative.
Reverse-biased Diode
A diode is said to be reverse-biased when the battery’s voltage is dropped completely. For silicon diodes, the reverse current is -20μA and for germanium, -50μA is the reverse current. The potential energy across the p-type material is negative and across the n-type material, the potential energy is positive.
Zero-biased Diode
When the diode is zero-biased, the voltage potential across the diode is zero.
Other More Diode's Application
- Diodes as a rectifier
- Diodes in the clipping circuit
- Diodes in clamping circuits
- Diodes in logical gates
- Diodes in reverse current protection
Diode logic (or diode-resistor logic) constructs AND and OR logic gates with diodes and resistors.
An active device (vacuum tubes in early computers, then transistors in diode–transistor logic) is additionally required to provide logical inversion (NOT) for functional completeness and amplification for voltage level restoration, which diode logic alone can't provide.
Since voltage levels weaken with each diode logic stage, multiple stages can't easily be cascaded, limiting diode logic's usefulness. However, diode logic has the advantage of utilizing only cheap passive components.
7 PN Diode internal structure at zero bias
Logic gates evaluate Boolean algebra, typically using electronic switches controlled by logical inputs connected in parallel or series. Diode logic can only implement OR and AND because inverters (NOT gates) require an active device.
Binary logic uses two distinct logic levels of voltage signals that may be labelled high and low. In this discussion, voltages close to +5 volts are high, and voltages close to 0 volts (ground) are low. The exact magnitude of the voltage is not critical, provided that inputs are driven by strong enough sources so that output voltages lie within detectably different ranges.
For active-high or positive logic, high represents logic 1 (true) and low represents logic 0 (false). However, the assignment of logical 1 and logical 0 to high or low is arbitrary and is reversed in active-low or negative logic, where low is logical 1 while high is logical 0. The following diode logic gates work in both active-high or active-low logic, however, the logical function they implement is different depending on what voltage level is considered active. Switching between active-high and active-low is commonly used to achieve a more efficient logic design.
In summary, if any input is high the output will be high, but only if all inputs are low will the output below:
|
Inputs |
Output |
||
|
Low |
||
|
High |
||
|
High |
||
|
High |
AND Gate Truth Table:
|
A |
B |
Output |
|
0 |
0 |
0 |
|
0 |
1 |
0 |
|
1 |
0 |
0 |
|
1 |
1 |
1 |
OR Gate Truth Table:
|
A |
B |
Output |
|
0 |
0 |
0 |
|
0 |
1 |
1 |
|
1 |
0 |
1 |
|
1 |
1 |
1 |
NOT Gate: Outputs the opposite of the input (also known as
an inverter). Truth Table:
|
A |
Output |
|
0 |
1 |
|
1 |
0 |
NAND Gate: Outputs false only if all inputs are true
(NOT-AND). Truth Table:
|
A |
B |
Output |
|
0 |
0 |
1 |
|
0 |
1 |
1 |
|
1 |
0 |
1 |
|
1 |
1 |
0 |
NOR Gate: Outputs true only if all inputs are false
(NOT-OR). Truth Table:
|
A |
B |
Output |
|
0 |
0 |
1 |
|
0 |
1 |
0 |
|
1 |
0 |
0 |
|
1 |
1 |
0 |
XOR Gate: Outputs true if inputs are different. Truth Table:
|
A |
B |
Output |
|
0 |
0 |
0 |
|
0 |
1 |
1 |
|
1 |
0 |
1 |
|
1 |
1 |
0 |
XNOR Gate: Outputs true if inputs are the same (NOT-XOR). Truth
Table:
|
A |
B |
Output |
|
0 |
0 |
1 |
|
0 |
1 |
0 |
|
1 |
0 |
0 |
|
1 |
1 |
1 |
Components:
- Battery: Provides the electrical energy.
- Resistor: Resists the flow of current (e.g., light bulb, LED, resistor).
- Connecting wires: Conduct the current.
Diagram:
Explanation:
In a series circuit, the components are connected one after another. The current flows through each component sequentially. The total resistance of the circuit is the sum of the individual resistances.
Example: If you have a 9V battery and a 10 ohm resistor, the current flowing through the circuit would be:
Current (I) = Voltage (V) / Resistance (R) = 9V / 10 ohms = 0.9 amps




Comments
Post a Comment