Resistances in Parallel

Electricity safety in electrical engineering prioritizes grounding, insulation coordination, overcurrent protection, arc-flash mitigation, lockout/tagout, and PPE to reduce shock, burn, and fire hazards in high-voltage and low-voltage installations through standards compliance and risk assessment.

What Is Electricity Safety?

Electricity safety is engineering practice to prevent shock, arc flash, and fire through design, controls, and standards.

✅ Implement grounding/earthing, bonding, and insulation coordination.

✅ Use overcurrent, residual current, and arc-fault protection.

✅ Apply NFPA 70E/IEC 60364, lockout/tagout, and arc-flash PPE.

Electricity Safety dangers involving voltages of greater than 50V are capable of producing heart fibrillation if they produce electric currents in body tissues which happen to pass through the chest area. The electrocution danger is mostly determined by the low conductivity of dry human skin. If skin is wet, or if there are wounds, or if the voltage is applied to electrodes which penetrate the skin, then even voltage sources below 40 V can be lethal if contacted. A DC circuit may be especially dangerous because it will cause muscles to lock around the wire. For a broader overview of common electrical hazards, the guide at dangers of electricity explains mechanisms of shock and injury.

Accidental contact with high voltage will usually result in severe injury or death. This can occur as a person's body provides a path for current flow causing tissue damage and heart failure. Other injuries can include burns from the arc generated by the accidental contact. These can be especially dangerous if the victims airways are affected. Injuries may also be suffered as a result of the physical forces exerted as people may fall fall from height or be thrown considerable distance. For context on regulatory and industry thresholds, see what is considered high voltage and how those limits are defined.

Electricity Safety

Depending on the short circuit current available at a switchgear line-up, a hazard is presented to maintenance and operating personnel due to the possibility of a high-intensity electric arc. Maximum temperature of an arc can exceed 10,000 kelvin, and the radiant heat, expanding hot air, and explosive vaporization of metal and insulation material can cause severe injury to unprotected workers. Such switchgear line-ups and high-energy arc sources are commonly present in electric power utility substations and generating stations and power lines, industrial plants and large commercial buildings. In the United States the National Fire Protection Association, has published a guideline standard NFPA 70E for evaluating and calculating arc flash hazard, and provides standards for the protective clothing required for electrical workers exposed to such hazards in the workplace. And even then, workers must still be careful. Understanding fault energy begins with the basics of a short circuit and how fault paths escalate incident energy.

While arc flash and arc blast are distinct, an arc fault can originate from insulation breakdown or wiring damage and quickly intensify conditions.

Explosion hazard

Even voltages insufficient to break down air can be associated with enough energy to ignite atmospheres containing flammable gases or vapours, or suspended dust. For example, air containing hydrogen gas or natural gas or gasoline vapor can be ignited by sparks produced by electrical apparatus fed by electricity lines or electricity power lines. Examples of industrial facilities with hazardous areas are petrochemical refineries, chemical plants, grain elevators, and some kinds of coal mines. In many environments, seemingly minor static electricity discharges are sufficient to ignite vapors if controls are inadequate.

Measures taken to prevent such explosions include:

• Intrinsic safety, which is apparatus designed to not accumulate enough stored energy to touch off an explosion
• Increased safety, which applies to devices using measures such as oil-filled enclosures to prevent contact between sparking apparatus and an explosive atmosphere
• Explosion-proof enclosures, which are designed so that an explosion within the enclosure cannot escape and touch off the surrounding atmosphere (this designation does not imply that the apparatus will survive an internal or external explosion).

In recent years standards for explosion hazard protection have become more uniform between European and North American practice. The "zone" system of classification is now used in modified form in U.S. National Electrical Code and in the Canadian electrical code. Intrinsic safety apparatus is now approved for use in North American applications, though the explosion-proof enclosures used in North America are still uncommon in Europe. For clarity on terminology used across these standards, consult this electricity terms glossary for consistent definitions.

The Electric Safety Home is a home in which the outlet plugs, electric cords, and each electricity plug and cord plug near sinks and water sources are GFCI protected. That makes them safe. Understanding the nature of a ground fault helps explain why GFCIs trip quickly to prevent shock.

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Ampere’s Law describes the relationship between magnetic fields and electric currents, a fundamental concept in electromagnetism. It explains how current produces a magnetic force, guiding the design of circuits, solenoids, coils, and transformers in electrical engineering.

What is Ampere’s Law?

Ampere's Law is a fundamental principle in electromagnetism that describes the relationship between electric current and the resulting magnetic field.

✅ It states that the magnetic field around a closed path is proportional to the electric current passing through it.

✅ It is a fundamental principle of electromagnetism, linking current and magnetic flux.

✅ Used in analyzing coils, solenoids, transformers, and magnetic circuits.

Named after the French physicist André-Marie Ampère, this powerful principle helps us understand the behaviour of magnetic fields generated by electric currents. It is crucial to develop the numerous technologies we use on a daily basis. Understanding Ampere's Law is easier when explored alongside related concepts in basic electricity, which provide the foundation for electrical theory.

The principle states that the line integral of a magnetic field (B) around a closed loop is equal to the product of the permeability of free space (μ₀) and the net electric current (I) passing through the loop. This can be mathematically represented as:

∮ B⋅dl = μ₀I

Ampere’s Law at a Glance

Ampere’s Law and Magnetism

The principle can be applied to determine the magnetic field around current-carrying wires and other conductive materials, as well as within various electrical systems. It is an essential part of Maxwell's equations, a set of four equations that serve as the foundation of classical electromagnetism. These equations relate electric and magnetic fields to their sources (electric charges and currents) and describe how they propagate through space. The connection between electricity and magnetism is central to electromagnetism, where Ampere’s Law works hand-in-hand with Faraday’s Law to explain induction.

It calculates magnetic fields through the Biot-Savart Law, a mathematical expression that relates the magnetic field produced by a steady electric current to the current's geometry. Both principles have specific applications, with the Biot-Savart Law being more suitable for cases with intricate current configurations. At the same time, it is typically employed when dealing with symmetrical setups.

Ampere’s Law has numerous real-life applications, especially in developing and understanding devices and systems that involve electromagnetism. For example, it is used in the design of transformers, inductors, and solenoids, as well as in various applications such as telecommunications systems, motors, and generators. By applying it, engineers can predict and control the magnetic fields generated in these devices, ensuring they function optimally and efficiently.

Gauss’ Law and Electric Fields Around a Circle of Radius

When studying electromagnetism, a common problem is analyzing the behavior of electric fields around a symmetric object, such as a circle of radius r or a sphere. Gauss’ Law is especially powerful in such cases, because it states that the electric flux through a closed surface is proportional to the net charge enclosed. This means the distribution of field lines can be calculated without solving complex integrals directly.

For a uniformly charged circle of radius r, the electric field at a point along the axis can be derived by considering the superposition of contributions from each charge element. The result reveals that the electric field depends on both the radius of the circle and the distance from the observation point. This demonstrates how Gauss’ Law simplifies problems with high symmetry.

Mathematically, the relationship is expressed as:

∮ E · dA = Q / ε₀

Here, E represents the vector field of the electric field, dA is the infinitesimal area vector on the closed surface, Q is the enclosed charge, and ε₀ is the permittivity of free space. By applying this principle, one can determine that electric fields radiate symmetrically outward from charges, with strength diminishing with distance according to the geometry of the surface considered.

The application of Gauss’ Law in analyzing a circle of radius r is connected to Ampere’s Law, as both emphasize symmetry and integration around closed paths. Where Ampere’s Law links magnetic fields to current, Gauss’ Law links electric fields to charge, and together they form part of Maxwell’s equations, the foundation of electromagnetism.

Relationship between Ampere's Law and Faraday's Law

The relationship between Ampere's Law and Faraday's Law of electromagnetic induction is apparent in the phenomenon of electromagnetic induction itself. When a changing magnetic field induces an electric current in a conductive material, the resulting magnetic field generated by this electric current, in turn, affects the overall magnetic field. It helps us understand how these interacting magnetic fields behave and influence each other.

Ampere's Law and its applications in various devices and systems enable numerous technological advancements. For instance, when designing motors and generators, engineers can utilize the principle to optimize the magnetic field within the device, resulting in higher efficiency and improved performance. Ampere’s Law is also linked to the behavior of capacitance and inductance, both of which are essential in circuits and energy storage systems.

In the telecommunications realm, it helps explain the propagation of electromagnetic waves in cables and antennas. It enables engineers to design systems that minimize signal loss and maximize data transfer rates, ensuring that our smartphones, computers, and other devices remain connected and up-to-date.

By understanding the magnetic field lines and the interaction between electric current and magnetic fields, Ampere's Law opens doors to scientific discovery and innovation in numerous fields. From determining the magnetic field at a distance to the thumb rule and hand rule applications, this fundamental principle plays a crucial role in shaping the world of electromagnetism and the technology that surrounds us.

Electromagnetism

It is a cornerstone of electromagnetism that helps us understand the relationship between electric current and how it creates a magnetic field. It is a vital component of Maxwell's equations and intricately connected to other principles, such as Faraday's Law and Biot-Savart's Law. Ampere's Law has numerous applications in real-life scenarios and is essential for the functioning of many devices and systems that rely on electromagnetism. Its significance in the development of technology cannot be overstated, as it continues to drive scientific discovery and innovation. For students exploring fundamentals, the history of concepts like what is electricity and its evolution in electricity history provides valuable context to Ampere’s discoveries.

How does Ampere’s Law relate to Faraday's Law and Biot-Savart Law?

They are all essential principles in electromagnetism that describe various aspects of the interaction between electric currents and magnetic fields. Although each addresses different aspects, these are interrelated, forming a more comprehensive understanding of electromagnetism.

It describes the relationship between an electric current and its generated magnetic field. Mathematically, it states that the line integral of the magnetic field (B) around a closed loop is proportional to the net electric current (I) passing through the loop:

∮ B⋅dl = μ₀I

Ampere’s Law is useful for calculating magnetic fields in highly symmetrical situations, such as around straight wires, loops, or solenoids.

Faraday's Law: Faraday's Law of Electromagnetic Induction describes how a changing magnetic field induces an electromotive force (EMF) in a conductor. Mathematically, it states that the induced EMF is proportional to the rate of change of the magnetic flux (ΦB) through a closed loop formed by the conductor:

EMF = -dΦB/dt

Faraday's Law is fundamental to understanding the operation of devices such as generators, transformers, and induction motors, which rely on converting mechanical and electrical energy.

The Biot-Savart Law calculates the magnetic field at any point in space due to a specific current distribution. Mathematically, it can be expressed as:

dB = (μ₀ / 4π) * (Idl × r̂) / r²

The Biot-Savart Law is particularly useful for calculating magnetic fields in complex current configurations without symmetry.

Ampere's Law and Biot-Savart Law

Ampere's Law and Biot-Savart Law: Both deal with the magnetic field generated by an electric current. While the first is useful for calculating magnetic fields in symmetric situations, the Biot-Savart Law applies to a wider range of configurations, including those with intricate geometries. It can be derived from the Biot-Savart Law for specific symmetric situations.

Ampere's Law and Faraday's Law

Ampere's Law and Faraday's Law: These laws are related through Maxwell's equations, which connect electric and magnetic fields. While the first deals with the magnetic field generated by a steady electric current, Faraday's Law deals with the induced EMF resulting from a changing magnetic field. Both laws contribute to our understanding of electromagnetic phenomena and play a role in operating devices that rely on electromagnetism.

The Biot-Savart Law enables us to determine the magnetic field generated by a specific current distribution. Faraday's Law describes how a changing magnetic field can induce an EMF. In cases where the magnetic field changes due to a varying current, the Biot-Savart Law can be used to calculate the magnetic field, and then Faraday's Law can be applied to determine the induced EMF.

All three are interconnected principles in electromagnetism, each addressing a specific aspect of the interaction between the electric current and the electric field. Together, these form a more comprehensive understanding of electromagnetic phenomena and provide a basis for analyzing and designing various devices and systems that rely on electromagnetism.

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Lenz’s Law is a principle of electromagnetic induction stating that induced current flows in a direction that opposes the change in magnetic flux producing it. This rule ensures energy conservation and explains how circuits, coils, generators, and transformers behave in changing fields.

What is Lenz’s Law?

Lenz’s Law, rooted in Faraday’s Law of Induction, states that the direction of an induced current or electromotive force (emf) always opposes the change in magnetic flux that produced it. This principle safeguards conservation of energy in electromagnetic systems.

✅ Explains opposing force in induced current and magnetic fields

✅ Fundamental to understanding circuits, transformers, and generators

✅ Practical in energy conversion, electric motors, and induction device

Lenz's Law, named after the Russian physicist Heinrich Lenz (1804-1865), is a fundamental principle in electromagnetism. It states that the direction of the induced electromotive force (emf) in a closed conducting loop always opposes the change in magnetic flux that caused it. This means that the induced current creates a magnetic field that opposes the initial change in magnetic flux, following the principles of conservation of energy. A strong grounding in basic electricity concepts makes it easier to see why Lenz’s Law is central to modern circuit design.

Understanding Lenz's Law enables us to appreciate the science behind various everyday applications, including electric generators, motors, inductors, and transformers. By exploring the principles of Lenz's Law, we gain insight into the inner workings of the electromagnetic world that surrounds us. Engineers use this principle when designing three-phase electricity systems and 3-phase power networks to maintain energy balance.

Lenz's Law, named after the Russian physicist Heinrich Lenz (1804-1865), is a fundamental principle that governs electromagnetic induction. It states that the induced electromotive force (emf) in a closed conducting loop always opposes the change in magnetic flux that caused it. In simpler terms, the direction of the induced current creates a magnetic field that opposes the initial change in magnetic flux. 

Lenz's Law is a fundamental law of electromagnetism that states that the direction of an induced electromotive force (EMF) in a circuit is always such that it opposes the change that produced it. Mathematically, Lenz's Law can be expressed as:

EMF = -dΦ/dt

Where EMF is the electromotive force, Φ is the magnetic flux, and dt is the change in time. The negative sign in the equation indicates that the induced EMF is in the opposite direction to the change in flux.

Lenz's Law is closely related to Faraday's Law of electromagnetic induction, which states that a changing magnetic field induces an EMF in a circuit. Faraday's Law can be expressed mathematically as:

EMF = -dΦ/dt

where EMF is the electromotive force, Φ is the magnetic flux, and dt is the change in time.

Ampere's Law and the Biot-Savart Law are also related to Lenz's Law, as they describe the behaviour of electric and magnetic fields in the presence of currents and charges. Ampere's Law states that the magnetic field around a current-carrying wire is proportional to the current and the distance from the wire. The Biot-Savart Law describes the magnetic field produced by a current-carrying wire or a group of wires. Because Lenz’s Law governs the behavior of induced currents, it directly complements Ampere’s Law and the Biot-Savart Law in explaining magnetic fields.

Together, these laws provide a complete description of the behaviour of electric and magnetic fields in various situations. As a result, they are essential for understanding the operation of electric motors, generators, transformers, and other devices.

To better understand Lenz's Law, consider the scenario of a bar magnet moving toward a coil of wire. When the magnet moves closer to the coil, the number of magnetic field lines passing through the coil increases. According to Lenz's Law, the polarity of the induced emf in the coil is such that it opposes the increase in magnetic flux. This opposition creates an induced field that opposes the magnet's motion, ultimately slowing it down. Similarly, when the magnet is moved away from the coil, the induced emf opposes the decrease in magnetic flux, creating an induced field that tries to keep the magnet in place.

The induced field that opposes the change in magnetic flux follows the right-hand rule. If we hold our right hand around the coil such that our fingers point in the direction of the magnetic field lines, our thumb will point in the direction of the induced current. The direction of the induced current is such that it creates a magnetic field that opposes the change in the magnetic flux.

The pole of the magnet also plays a crucial role in Lenz's Law. When the magnet's north pole moves towards the coil, the induced current creates a magnetic field that opposes the north pole's approach. Conversely, when the magnet's south pole moves towards the coil, the induced current creates a magnetic field that opposes the south pole's approach. The direction of the induced current follows the right-hand rule, as we discussed earlier.

It is related to Faraday's Law of Electromagnetic Induction, which explains how a changing magnetic field can induce an electromotive force (emf) in a conductor. Faraday's Law mathematically describes the relationship between the induced electromotive force (emf) and the rate of change of magnetic flux. It follows Faraday's Law, as it governs the direction of the induced emf in response to the changing magnetic flux. To fully understand how electromagnetic induction works, it is helpful to see how Faraday’s discoveries laid the foundation for Lenz’s Law.

It is also related to the phenomenon of eddy currents. Eddy currents are loops of electric current induced within conductors by a changing magnetic field. The circulating flow of these currents generates their magnetic field, which opposes the initial magnetic field that created them. This effect is in line with Lenz's Law and has practical applications, such as in the braking systems of trains and induction cooktops.

Lenz's Law has numerous practical applications in our daily lives. For example, it plays a significant role in the design and function of electric generators, which convert mechanical energy into electrical energy. In a generator, a rotating coil experiences a changing magnetic field, resulting in the generation of an electromotive force (emf). The direction of this induced emf is determined by Lenz's Law, which ensures that the system conserves energy. Similarly, electric motors operate based on Lenz's Law. In an electric motor, the interaction between the magnetic fields and the induced electromotive force (emf) creates a torque that drives the motor. In transformers, including 3-phase padmounted transformers, Lenz’s Law explains why flux changes are controlled for efficiency and safety.

Lenz's Law is an essential concept in the design of inductors and transformers. Inductors are electronic components that store energy in their magnetic field when a current flows through them. They oppose any change in the current, following the principles of Lenz's Law. Transformers, which are used to transfer electrical energy between circuits, utilize the phenomenon of electromagnetic induction. By understanding it, engineers can design transformers.

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The voltage drop formula is V = I × R, where V represents the voltage drop, I represents the current in amperes, and R represents the resistance in ohms. It calculates the amount of voltage lost through a conductor and is essential for designing safe and efficient electrical systems.

What is Voltage Drop Formula?

A voltage drop formula can help you manually calculate the voltage drop in cables under full load in branch circuits. It does not matter if you are working with copper or aluminum conductors. To accurately calculate the voltage drop for a given cable size, length, and current, you need to know the resistance of the type of cable you’re using. 

✅ V = I × R for DC circuits

✅ Accounts for impedance in AC circuits

✅ Helps ensure safe, efficient electrical design

Use our voltage drop calculator to quickly determine wire size, conductor efficiency, and line loss for safer, more reliable electrical installations.

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To determine voltage drop in an electrical system, engineers and electricians use a standard formula that accounts for conductor resistance, current, and circuit length. The National Electrical Code (NEC) provides guidelines for the maximum voltage drop allowed in various installations to ensure efficiency and safety. For both single-phase and three-phase circuits, excessive voltage drop can lead to poor equipment performance and energy loss. To simplify calculations, a voltage drop calculator can quickly assess whether a circuit meets NEC recommendations and optimize conductor sizing accordingly. You can learn more about how electrical resistance affects circuits in our detailed voltage drop guide, which explains causes, calculations, and solutions for safe, efficient power distribution.

DC / single phase calculation

The voltage drop V in volts (V) is equal to the wire current I in amps (A) times 2 times one way wire size length L in feet (ft) times the wire resistance per 1000 feet R in ohms (Ω/kft) divided by 1000:

Vdrop (V) = Iwire (A) × Rwire(Ω)

= Iwire (A) × (2 × L(ft) × Rwire(Ω/kft) / 1000(ft/kft))

The voltage drop V in volts (V) is equal to the wire current I in amps (A) times 2 times one way wire length L in meters (m) times the wire resistance per 1000 meters R in ohms (Ω/km) divided by 1000:

Vdrop (V) = Iwire (A) × Rwire(Ω)

= Iwire (A) × (2 × L(m) × Rwire (Ω/km) / 1000(m/km))

3 phase calculation

The line-to-line voltage drop V in volts (V) is equal to the square root of 3 times the wire current I in amps (A) times one-way wire length L in feet (ft) times the wire resistance per 1000 feet R in ohms (Ω/kft) divided by 1000:

Vdrop (V) = √3 × Iwire (A) × Rwire (Ω)

= 1.732 × Iwire (A) × (L(ft) × Rwire (Ω/kft) / 1000(ft/kft))

The line-to-line voltage drop V in volts (V) is equal to the square root of 3 times the wire current I in amps (A) times one-way wire length L in meters (m) times the wire resistance per 1000 meters R in ohms (Ω/km) divided by 1000:

Vdrop (V) = √3 × Iwire (A) × Rwire (Ω)

= 1.732 × Iwire (A) × (L(m) × Rwire (Ω/km) / 1000(m/km))

Wire diameter calculations

The n gauge wire diameter, dn in inches (in), is equal to 0.005in times 92 raised to the power of 36 minus gauge number n, divided by 39:

dn (in) = 0.005 in × 92(36-n)/39

The n gauge wire diameter dn in millimetres (mm) is equal to 0.127mm times 92 raised to the power of 36 minus gauge number n, divided by 39:

dn (mm) = 0.127 mm × 92(36-n)/39

Wire cross-sectional area calculations

The n gauge wire's cross-sectional area An in kilo-circular mils (kcmil) is equal to 1000 times the square wire diameter d in inches (in):

An (kcmil) = 1000×dn2 = 0.025 in2 × 92(36-n)/19.5

The n gauge wire's cross-sectional area An in square inches (in2), is equal to pi divided by 4 times the square wire diameter d in inches (in):

An (in2) = (π/4)×dn2 = 0.000019635 in2 × 92(36-n)/19.5

The n gauge wire's cross-sectional area, An, in square millimetres (mm2), is equal to pi divided by 4 times the square wire diameter d in millimetres (mm):

An (mm2) = (π/4)×dn2 = 0.012668 mm2 × 92(36-n)/19.5

Wire resistance calculations

The n gauge wire resistance R in ohms per kilofeet (Ω/kft) is equal to 0.3048×1000000000 times the wire's resistivity ρ in ohm-meters (Ω·m) divided by 25.42 times the cross-sectional area An in square inches (in2):

Rn (Ω/kft) = 0.3048 × 109 × ρ(Ω·m) / (25.42 × An (in2))

The n gauge wire resistance R in ohms per kilometre (Ω/km) is equal to 1000000000 times the wire's resistivity ρ in ohm-meters (Ω·m) divided by the cross-sectional area An in square millimetres (mm2):

Rn (Ω/km) = 109 × ρ(Ω·m) / An (mm2)

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Harmonic distortion is the deviation from the ideal electrical waveform caused by nonlinear loads. It impacts power quality, increases heat in equipment, and can lead to system inefficiencies. Monitoring and mitigation are essential in industrial electrical systems.

What is Harmonic Distortion?

Harmonic distortion is not a new phenomenon in power systems. Concern over distortion has fluctuated several times throughout the history of AC electric power systems.

✅ Reduces overall power quality and system reliability

✅ Can damage equipment and increase heat generation

✅ Requires monitoring to ensure system efficiency and safety

In the 1930s and 1940s, the primary sources were transformers, with the primary problem being inductive interference with open-wire telephone systems. Early arc lighting caused similar concern due to its harmonic content, just as today’s electronic power converters do.

Today, nonlinear devices like variable frequency drives (VFDs), arc furnaces, computer power supplies, and LED lighting introduce significant harmonic distortion into electrical systems. Nonlinear devices do not draw current in a linear relationship to voltage, which distorts the sinusoidal waveform and introduces harmonic currents. Harmonic distortion is one of the many issues covered in our comprehensive Power Quality resource channel, which explores causes, effects, and solutions.

Why It Matters

• Harmonics degrade power quality

• Increase energy losses and heat in conductors and transformers

• Lead to premature failure of motors and sensitive electronics

• Interfere with communication lines

In contrast, voltage sags and interruptions are nearly universal to every feeder and represent the most numerous and significant power quality deviations. The end-user sector suffers more from harmonic problems than the utility sector. Industrial users with adjustable speed drives, arc furnaces, induction furnaces, and similar equipment are significantly more susceptible to problems caused by harmonic distortion. To understand the relationship between harmonics and apparent energy flow, see our explanation of Apparent Power vs Real Power.

A good assumption for most utilities in the United States is that the sine wave voltage generated in central power stations is very good. In most areas, the voltage found on transmission systems typically has much less than 1% distortion. However, the distortion increases as the load approaches. At some loads, the current waveforms barely resemble a sine wave. Electronic power converters can chop the current into seemingly arbitrary waveforms. Managing nonlinear loads often requires Power Factor Correction to reduce harmonic effects and improve efficiency.

Industry Standards

• IEEE 519: Sets recommended harmonic limits for both voltage and current.

• IEC 61000-4-7: Defines methods of measuring harmonics and interharmonics.

Harmonic Distortion and Nonlinear Devices

Harmonic distortion is caused by nonlinear devices in the power system. A nonlinear device is one in which the current is not proportional to the applied voltage. Figure 1 illustrates this concept using the case of a sinusoidal voltage applied to a simple nonlinear resistor, where the voltage and current vary according to the curve shown. While the applied voltage is perfectly sinusoidal, the resulting current is distorted. Increasing the voltage by a few percent may cause the current to double and exhibit a different waveform. You can calculate your system’s power quality impact using our Apparent Power Calculator for precise performance metrics.

This is the source of most harmonic distortion in a power system. Figure 1 illustrates that any periodic, distorted waveform can be expressed as a sum of sinusoids. When a waveform is ideal from one cycle to the next, it can be represented as a sum of pure sine waves in which the frequency of each sinusoid is an integer multiple of the fundamental frequency of the distorted wave. This multiple is called a harmonic of the fundamental, hence the name of this subject matter. The sum of sinusoids is referred to as a Fourier series, named after the great mathematician who discovered the concept. Nonlinear loads like VFDs and arc furnaces can affect grounding; learn more in our guide to Electrical Grounding.

Fig. 1. Current distortion caused by nonlinear resistance

Voltage and Current Distortion

The term "harmonics" is often used by itself without further qualification. Generally, it could mean one of the following three:

1. The harmonic voltages are too great (the voltage is too distorted) for the control to properly determine firing angles.

2. The harmonic currents are too great for the capacity of some devices in the power supply system, such as transformers, and the machine must be operated at a lower than rated power.

3. The harmonic voltages are too great because the harmonic currents produced by the device are too great for the given system condition.

Clearly, there are separate causes and effects for voltages and currents, as well as some relationship between them. Thus, the term harmonics by itself is inadequate to describe a problem definitively. Nonlinear loads appear to be sources of harmonic current, injecting harmonic currents into the power system. For nearly all analyses, it is sufficient to treat these harmonic-producing loads simply as current sources. There are exceptions to this as described later.

Fig 2. Harmonic currents flowing through the system impedance result in harmonic voltages at the load.

Voltage distortion is the result of distorted currents passing through the linear, series impedance of the power delivery system, as illustrated in Fig. 2. Although assuming that the source bus is ultimately a pure sinusoid, there is a nonlinear load that draws a distorted current. The harmonic currents passing through the system's impedance cause a voltage drop for each harmonic. This results in voltage harmonics appearing at the load bus. The amount of voltage distortion depends on the impedance and the current. Assuming the load bus distortion stays within reasonable limits (e.g., less than 5%), the amount of harmonic current produced by the load is generally constant.

While the load current harmonics ultimately cause voltage distortion, it is worth noting that the load has no control over the voltage distortion. The same load put in two different locations on the power system will result in two different voltage distortion values. Recognition of this fact is the basis for the division of responsibilities for harmonic control that is found in standards such as IEEE Std 519-1992.

• Control over the amount of harmonic current injected into the system occurs at the end-use application.

• Assuming the harmonic current injection is within reasonable limits, the control over voltage distortion is exercised by the entity that controls the system impedance, typically the utility.

One must be careful when describing harmonic distortion phenomena, as there are distinct differences between the causes and effects of harmonic voltages and currents. The use of the term harmonics should be qualified accordingly. By popular convention in the power industry, the term is used by itself most of the time when referring to load apparatus, indicating that the speaker is referring to the harmonic currents. When referring to the utility system, the voltages are generally the subject. For systems affected by harmonic-induced overheating, understanding Capacitor Bank applications is essential for voltage support and harmonic filtering. For in-depth harmonic analysis, explore our guide to using a Power Quality Analyzer to identify waveform distortion and power anomalies.

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Windmills for electricity use wind energy to generate clean, renewable power. These wind turbines convert kinetic energy into electrical energy, reducing carbon emissions and dependence on fossil fuels. 

What are Windmills for Electricity?

Windmills for electricity are modern devices that transform kinetic wind energy into electrical power.

✅ Harness renewable energy for clean power

✅ Reduce carbon footprint and dependence on fossil fuels

✅ Support sustainable power generation worldwide

Windmills for electricity are part of a broader shift toward renewable energy, providing clean alternatives to fossil fuels for homes, businesses, and utilities.

History of Windmills

Windmills for electricity - Mankind has been harnessing the wind's energy for many years. From Holland to traditional farms around the world, windmills were used in the past for pumping water through primitive irrigation systems or to grind grain. Then, the wind turned large "sails" that were connected by a long vertical shaft, which was attached to a grinding machine or a wheel that turned and drew water from a well. Today's turbines harness the energy of the wind to turn large metal blades, which in turn spin a generator that produces electric power. Alongside wind, other renewable energy sources like solar, biomass, and tidal energy are shaping a diversified and sustainable energy future.

From the mid-1970s to the mid-1980s, the United States government collaborated with industry to advance windmill technology for power generation and enable the development of large commercial wind turbines. NASA led this effort at the Lewis Research Center in Cleveland, Ohio, and it was an extraordinarily successful government research and development activity.

National Science Foundation

With funding from the National Science Foundation and later the Department of Energy (DOE), a total of 13 experimental wind turbines were put into operation, including four major wind turbine designs. This research and development program pioneered many of the multi-megawatt turbine technologies in use today, including steel tube towers, variable-speed generators, composite blade materials, partial-span pitch control, as well as aerodynamic, structural, and acoustic engineering design capabilities. The large Windmills For Electricity developed under this effort set several world records for diameter and power output. The Mod-2 wind turbine cluster produced a total of 7.5 megawatts of power in 1981. Government incentives, such as alternative energy tax credits, have played a major role in expanding wind power adoption across North America.

Wind Turbine Technology

In 1987, the Mod-5B was the largest single wind turbine operating in the world with a rotor diameter of nearly 100 meters and a rated power of 3.2 megawatts. It demonstrated an availability of 95 percent, an unparalleled level for a new first-unit wind turbine. The Mod-5B featured the first large-scale variable-speed drive train and a sectioned, two-blade rotor, which enabled easy transport of the blades.

Later, in the 1980s, California provided tax rebates for ecologically harmless wind turbines. These rebates helped fund the first major deployment of wind power for the utility grid. These turbines gathered in large wind parks such as at Altamont Pass, would be considered small and uneconomical by modern wind power development standards.

In the 1990s, as aesthetics and durability became more important, turbines were placed atop steel or reinforced concrete towers. Small generators are connected to the ground tower, and then the tower is raised into position. Larger generators are hoisted into position atop the tower, and a ladder or staircase is located inside the tower to allow technicians to reach and maintain the generator.

Originally, wind turbines were built right next to where their power was needed. With the availability of long-distance electric power transmission, wind generators are now often on wind farms in windy locations, and huge ones are being built offshore, sometimes transmitting power back to land using high-voltage submarine cable. Since wind turbines are a renewable means of generating power, they are being widely deployed, but their cost is often subsidized by taxpayers, either directly or through renewable energy credits. Much depends on the cost of alternative energy sources. The cost of wind generators per unit of power has been decreasing by about 4% per year.

Modern Wind Turbines

The most modern generations of Windmills for electricity are more properly called wind turbines, or wind generators, and are primarily used to generate electric power. Modern windmills are designed to harness the energy of the wind and convert it into electric energy. The largest wind turbines can generate up to 6 MW of power (for comparison, a modern fossil fuel power plant generates between 500 and 1,300 MW). Many large-scale renewable energy projects now combine wind farms with solar and storage systems, ensuring reliable, clean power for communities worldwide.

Small wind turbines can generate as little as a few kilowatts, while larger models produce up to 100 kilowatts or more, depending on design and location. These devices capture moving air, and as wind turbines operate, the kinetic energy generated can be used directly or sent into the electrical grid. On a utility scale, wind farms combine many large turbines to deliver massive amounts of energy, powering thousands of homes and businesses. This range of applications, from residential to industrial, demonstrates the versatility of wind technology in meeting diverse energy needs.

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