Capacitors in Series Explained

By R.W. Hurst, Editor


Capacitors in series lower the total capacitance but increase voltage handling. This configuration is widely used in electronics, circuit design, and energy storage to balance voltage and improve reliability.

 

What are Capacitors in Series?

Capacitors in series describe a circuit configuration where capacitors are connected end to end, affecting capacitance and voltage distribution.

✅ The total capacitance is always less than the smallest capacitor value

✅ Voltage divides across each capacitor based on its capacitance

✅ Improves voltage rating of circuits while lowering equivalent capacitance

They play a critical role in various electronic applications, and understanding their characteristics, advantages, and potential drawbacks is essential for designing and implementing successful circuits. By mastering the concepts of capacitance, voltage distribution, and energy storage, one can leverage capacitors in series to create optimal circuit designs. To fully understand how capacitors (caps) behave in different setups, it helps to compare Capacitance in Parallel with series connections and see how each affects circuit performance.


 

Capacitors are fundamental components in electronic circuits, and their applications are vast, ranging from simple timing circuits to sophisticated filtering applications. This article delves into the intricacies of caps connected in series, highlighting their characteristics, advantages, and potential drawbacks.

To understand capacitors in series, it's essential first to grasp the concept of capacitance, which represents a capacitor's ability to store electric charge. Caps consist of two conductive plates separated by a dielectric material that can store energy when an applied voltage is present. The amount of energy stored depends on the capacitance value, voltage rating, and the dielectric material used. Engineers often study Capacitance and its capacitance definition to calculate charge storage and predict how components will interact in series circuits. 

When caps are connected in series, their individual capacitance values contribute to the total equivalent capacitance. The series connection is achieved when the positive plate of one capacitor is connected to the negative plate of the subsequent capacitor. This forms a continuous path for current flow, creating a series circuit.

Calculating the total capacitance for capacitors in series is different from parallel capacitors. In a series connection, the reciprocal of the total equivalent capacitance is equal to the sum of the reciprocals of the individual capacitance values. Mathematically, this is represented as:

1/C_total = 1/C1 + 1/C2 + 1/C3 + ... + 1/Cn

Where C_total is the total equivalent capacitance, and C1, C2, C3, ... Cn are the individual capacitance values of the number of caps connected in series.

In a series connection, the electric charge stored in each capacitor is the same. However, the voltage across each capacitor varies depending on its capacitance. According to Kirchhoff's voltage law, the sum of voltages across individual capacitors must equal the applied voltage. Thus, higher capacitance values will have lower voltage drops, while lower capacitance values will have higher voltage drops.

There are both advantages and disadvantages to connecting capacitors in series. On the plus side, the voltage rating of the series connection increases, allowing the circuit to handle higher voltage levels without risking damage to the caps. This feature is particularly useful in high-voltage capacitors in series applications. Alongside capacitors, Amperes Law and Biot Savart Law provide deeper insight into the electromagnetic principles that govern current and voltage distribution.

However, there are also drawbacks to this arrangement. The total equivalent capacitance decreases as more capacitors are added to the series, which may limit the energy storage capabilities of the circuit. Moreover, in the event of a capacitor failure, the entire series connection is compromised.

Different capacitor types and values can be combined in a series configuration, but care must be taken to consider each capacitor's voltage ratings and tolerances. For instance, mixing capacitors with different dielectric materials may lead to uneven voltage distribution and reduced overall performance. Since Capacitors are essential to energy storage and timing circuits, learning their behavior in a Capacitors in Series arrangement is key for advanced electronics design.

Determining the total energy stored in a series connection of caps involves calculating the energy stored in each individual capacitor and then summing those values. The formula for energy storage in a capacitor is:

E = 0.5 * C * V^2

Where E is the energy stored, C is the capacitance, and V is the voltage across the capacitor. Calculating each capacitor's energy and adding the results can determine the total energy stored in the series connection.

Compared with parallel configurations, the total capacitance increases in parallel connections while it decreases in series. In parallel, the total capacitance is the sum of the individual capacitance values:

C_total = C1 + C2 + C3 + ... + Cn

A crucial aspect of working with capacitors in series is charge distribution. As mentioned earlier, the electric charge stored in each capacitor is the same, but the voltage distribution varies depending on the capacitance values. This characteristic influences the circuit's behaviour and must be considered when designing complex electronic systems. Uneven voltage distribution can affect the entire system's performance, making choosing caps with appropriate capacitance values and voltage ratings for a specific application is vital.

Another important factor to consider is the plate area. In general, caps with larger plate areas have higher capacitance values. Therefore, when connecting capacitors in series, it is essential to evaluate how the plate area of each capacitor influences the overall capacitance of the series connection. Understanding these factors will enable engineers and hobbyists to make informed decisions when designing and constructing electronic circuits.

Capacitors in series are versatile and valuable configurations for various electronic applications. By understanding the principles of capacitance, voltage distribution, energy storage, and the influence of dielectric materials, one can harness the full potential of capacitors connected in series. Additionally, being mindful of the advantages and disadvantages of this configuration and considering the compatibility of different capacitor types and values will enable the creation of efficient, reliable, and effective electronic circuits. As electronics evolve, they will remain critical in developing innovative devices and systems. A solid foundation in Basic Electricity makes it easier to grasp why capacitors in series lower overall capacitance but increase voltage handling.

 

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Norton's Theorem

Norton’s Theorem simplifies electrical circuit analysis by reducing any complex linear network to an equivalent current source in parallel with a resistor, enabling easier calculation of load current, evaluation of resistance, and solving practical problems.

 

What is Norton’s Theorem?

Norton’s Theorem states that any linear electrical network with sources and resistances can be reduced to an equivalent current source in parallel with a single resistor.

✅ Represents complex circuits as a simple current source and resistor

✅ Simplifies load current and resistance calculations

✅ Enhances circuit analysis for power systems and electronics

 

Understanding Norton's Theorem

Norton's Theorem is a foundational principle in electrical engineering, used to simplify the analysis of linear electronic circuits. This theorem, often taught alongside Thevenin's Theorem, provides a practical method for reducing complex circuits into a manageable form. The main insight of Norton's Theorem is that any two-terminal linear circuit, regardless of its internal complexity, can be represented by an ideal current source in parallel with a single resistor. This transformation does not alter external circuit behavior, making calculations and predictions about circuit performance far more straightforward. To fully grasp circuit simplification methods like Norton’s Theorem, it helps to start with a foundation in basic electricity.

Norton’s Theorem states that any linear electrical network can be simplified into a Norton equivalent circuit, making analysis more manageable. This representation is similar to an equivalent circuit consisting of a single current source and parallel resistance, allowing engineers to determine load behavior with ease. By calculating the total resistance of the network and combining it with the Norton current, complex problems become straightforward, enabling accurate predictions of circuit performance in both educational and real-world applications.

 

How Norton's Theorem Works

To use Norton's Theorem, engineers follow a step-by-step process:

  1. Identify the portion of the circuit to simplify: Usually, this means the part of the circuit as seen from a pair of terminals (often where a load is connected).

  2. Find the Norton current (IN): This is the current that would flow through a short circuit placed across the two terminals. It's calculated by removing the load resistor and finding the resulting current between the open terminals.

  3. Calculate the Norton resistance (RN): All independent voltage and current sources are deactivated (voltage sources are shorted, current sources are open-circuited), and the resistance seen from the open terminals is measured.

  4. Draw the Norton equivalent: Place the calculated current source (IN) in parallel with the calculated resistor (RN) between the terminals in question.

  5. Reconnect the load resistor: The circuit is now simplified, and analysis (such as calculating load current or voltage) is far easier.

Calculating Norton resistance often relies on principles such as Ohm’s Law and electrical resistance.

 

Why Use Norton's Theorem?

Complex electrical networks often contain multiple sources, resistors, and other components. Calculating the current or voltage across a particular element can be difficult without simplification. Norton's Theorem allows engineers to:

  • Save time: By reducing a circuit to source and resistance values, repeated calculations for different load conditions become much faster.

  • Enhance understanding: Seeing a circuit as a source and parallel resistor clarifies key behaviors, such as maximum power transfer.

  • Test different scenarios: Engineers can quickly swap different load values and immediately see the effect without having to recalculate the entire network each time.

Understanding how current behaves in different networks connects directly to the study of direct current and alternating current.

 

Comparison to Thevenin’s Theorem

Norton's Theorem is closely related to Thevenin's Theorem. Thevenin's approach uses a voltage source in series with a resistor, while Norton's uses a current source in parallel with a resistor. The two equivalents can be converted mathematically:

  • Thevenin equivalent resistance (RTH) = Norton equivalent resistance (RN)
  • Norton current (IN) = Thevenin voltage (VTH) divided by Thevenin resistance (RTH)
  • Thevenin voltage (VTH) = Norton current (IN) times resistance (RN)

Engineers applying Norton’s Theorem also draw on related concepts such as equivalent resistance and impedance to analyze circuits accurately.

 

Real-World Example

Suppose you need to know the current flowing through a sensor in a larger industrial power distribution board. The network supplying the sensor includes many resistors, switches, and sources. Applying Norton's Theorem, you can remove the sensor and find:

  1. The short-circuit current across its terminals (Norton current)
  2. The combined resistance left in the circuit (Norton resistance)

Once you reconnect the sensor and know its resistance, you can easily analyze how much current it will receive, or how it will affect circuit performance under different conditions.

For a deeper understanding, exploring electricity and magnetism reveals how fundamental laws, such as Faraday’s Law and Ampere’s Law, support the theory behind circuit transformations.

 

Applications of Norton's Theorem

  • Power system analysis: Used by utility engineers to study how changes in distribution, like maintenance or faults, impact circuit behavior.

  • Electronic device design: Common in transistors, op-amps, and other components to simplify input and output circuit analysis.

  • Fault diagnosis and protection: Helps quickly estimate fault currents for setting up protective devices in grids.

  • Education: Essential in electrical engineering curricula to develop problem-solving skills.

 

Limitations of Norton's Theorem

While powerful, Norton's Theorem is limited to linear circuits and cannot be directly applied to circuits with non-linear components (such as diodes or transistors in their non-linear regions). Additionally, it is only applicable between two terminals of a network; for systems with more terminals, additional techniques are required.

Norton's Theorem remains a valuable tool for engineers and students, offering clarity and efficiency in analyzing complex circuits. By transforming intricate arrangements into simple source-resistor pairs, it enables faster design iterations, troubleshooting, and optimized system performance. Whether you're analyzing a power distribution panel or designing integrated circuits, understanding and applying Norton's Theorem is an essential skill in the electrical field.

 

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Resistance Formula Explained

The resistance formula, R = V/I, shows how voltage and current determine opposition in a circuit. Central to Ohm’s Law, it is widely applied in electronics, power distribution, and engineering to calculate resistance, ensure efficiency, and design reliable electrical systems.

 

What is a Resistance Formula?

The resistance formula is a vital tool in understanding and optimizing electrical circuits. By analyzing the interplay between Ohm's law, conductor material, wire length, cross-sectional area, and temperature, we can manipulate Resistance to improve circuit performance. Balancing these factors ensures the efficient flow of electrons, minimizes energy loss, and maximizes the effectiveness of our electrical devices.

✅ R = V/I links voltage, current, and resistance

✅ Essential for circuit analysis and design

✅ Applied in electronics, power systems, and physics

 

Electrical circuits are essential for powering our daily lives, and understanding the factors that influence their performance is key to optimizing their efficiency. A critical aspect of electrical circuits is the Resistance they encounter, which directly affects the flow of electrons. Based on Ohm's law, the formula helps us analyze and manipulate various elements within a circuit. Topics like electrical resistance and the unit of electrical resistance expand on how opposition to current flow is measured and applied in engineering.

The flow of charge in any conductor depends on material properties and circuit design, where individual resistances combine differently depending on series or parallel circuit arrangements. According to law resistance principles, the total parallel resistance is always less than the smallest branch, and values are measured as resistance in ohms. Materials with the smallest resistivities like copper conduct efficiently, though their performance is affected by the temperature coefficient of resistivity, which alters conduction as heat rises. For visual examples and diagrams, resources such as Wikimedia Commons provide helpful illustrations.

 

Ohm's Law

Ohm's law is fundamental to understanding electrical circuits. It states that the Voltage across a conductor is directly proportional to the electric Current passing through it, and the constant of proportionality is the electrical Resistance. In mathematical terms, Ohm's law can be expressed as V = IR, where V is the Voltage, I is the electric Current, and R is the Resistance. Related principles, including Ampere’s Law and the Biot-Savart Law, further explain how current and magnetic fields interact with resistance in circuits.

The formula R = ρ(L/A) is derived from Ohm's law and describes how R depends on the conductor's material, length (L), and cross-sectional area (A). The resistivity (ρ) is a property unique to the conductor material and represents its ability to impede the flow of electrons. Different materials, such as copper or aluminum, have different resistivities, affecting the overall electrical R.

Wire length and cross-sectional area play a significant role in determining a conductor's R. As the wire length increases, so does the R, as electrons face more obstacles. Conversely, increasing the cross-sectional area reduces R, allowing more electrons to flow through the conductor simultaneously. This inverse relationship between R and cross-sectional area is vital in designing circuits to minimize energy loss and optimize efficiency.

 

Various factors influence the resistivity of conductor material. For instance, impurities in the material can hinder electron flow, thereby increasing resistivity. Additionally, the arrangement of atoms within the material's lattice structure affects the ease with which electrons can pass. Finally, the temperature coefficient is crucial, as fluctuations can alter resistivity. Generally, R increases with higher temperatures as atoms vibrate more and impede electron flow.

Resistance and conductance differ in their relationship to the flow of electrons. While R quantifies the opposition a conductor presents to the flow of electrons, conductance represents the ease with which electrons can pass. Mathematically, conductance (G) is the reciprocal of Resistance (R), and is measured in Siemens (S):

G = 1/R

The formula can be used to calculate power dissipation in a circuit. Power (P) is the product of Voltage (V) and current (I): P = VI. Using Ohm's law, we can substitute V = IR into the power formula to obtain P = I^2R. This equation demonstrates that higher R results in greater power dissipation, manifesting as heat. Hence, managing R is essential in preventing energy loss and maintaining circuit efficiency.

Ohm's law defines a mathematical relationship involving V, R, and current (I) within an electrical component. Ohm, denoted by the Greek letter omega (Ω), is the unit of measurement for R. Furthermore, Ohm's law can derive a power equation by computing electrical power, quantified in watts. Subsequently, Gustav Kirchhoff built upon Ohm's foundational work and introduced Kirchhoff's rules, two equalities addressing current and Voltage in an electric circuit model.

Ohm's law outlines the fundamental principles of electrical circuits, highlighting the interdependence between voltage, current, and resistance. This relationship can be expressed in three different formulas:

V = I × R (Voltage equals Current multiplied by Resistance)
R = V / I (Resistance equals Voltage divided by Current)
I = V / R (Current equals Voltage divided by Resistance)

These formulas illustrate the interconnection of voltage, current, and resistance in electrical circuits. By manipulating these relationships, we can analyze the behaviour of circuits, troubleshoot issues, and optimize efficiency.

The significance of Ohm's law extends beyond its mathematical representation. It forms the basis for understanding various electrical phenomena, including power dissipation, energy consumption, and the impact of R on the performance of electrical components. The role of resistance is closely tied to capacitance and inductance, which determine energy storage and reactance in alternating current systems.

As we explore the vast applications of electrical circuits, understanding the formula allows us to make informed decisions in choosing conductor materials, adjusting wire length and cross-sectional area, and considering temperature fluctuations. With an understanding of how these factors interact, we can continue to innovate, create, and harness the power of electricity to achieve a brighter future.

 

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Electrical Units Explained

Electrical units measure various aspects of electricity, such as voltage (volts), current (amperes), resistance (ohms), and power (watts). These standard units are crucial in electrical engineering, circuit design, energy monitoring, and ensuring the safe operation of electrical systems.

 

What are Electrical Units?

Electrical units are standardized measures used to quantify electrical properties in circuits and systems.

✅ Measure voltage, current, resistance, power, and energy

✅ Used in electrical engineering, testing, and design

✅ Support safe and efficient electrical system operations

Electrical units are standardized measurements that describe various aspects of electricity, such as current, voltage, resistance, and power. These units, like amperes for current and volts for voltage, help quantify the behavior and interaction of systems. By understanding electrical units, professionals can assess performance, design circuits, and ensure safety across different applications. These electrical units play a crucial role in the functioning of everything from household appliances to industrial machinery, making them fundamental in engineering and everyday technology.

In common electricity systems, various electrical units of measure, such as magnetic field, are used to describe how electricity flows in the circuit. For example, the unit of resistance is the ohm, while the unit of time is the second. These measurements, often based on SI units, help define the phase angle, which describes the phase difference between current and voltage in AC circuits. Understanding these electrical units is critical for accurately analyzing performance in both residential and industrial applications, ensuring proper function and safety.

 

Ampere

The ampere is the unit of electric current in the SI, used by both scientists and technologists. Since 1948, the ampere has been defined as the constant current that, if maintained in two straight, parallel conductors of infinite length and negligible circular cross-section, and placed one meter apart in a vacuum, would produce between these conductors a force equal to 2 × 10^7 newtons per meter of length. Named for the 19th-century French physicist André-Marie Ampere, it represents a flow of one coulomb of electricity per second. A flow of one ampere is produced in a resistance of one ohm by a potential difference of one volt. The ampere is the standard unit of electric current, playing a central role in the flow of electricity through electrical circuits.

 

Coulomb

The coulomb is the unit of electric charge in the metre-kilogram—second-ampere system, the basis of the SI system of physical electrical units. The coulomb is defined as the quantity of electricity transported in one second by a current of one ampere. Named for the I8th—I9th-century French physicist.

 

Electron Volt

A unit of energy commonly used in atomic and nuclear physics, the electron volt is equal to the energy gained by an electron (a charged particle carrying one unit of electronic charge when the potential at the electron increases by one volt. The electron volt equals 1.602 x IO2 erg. The abbreviation MeV indicates 10 to the 6th (1,000,000) electron volts, and GeV, 10 to the 9th (1,000,000,000). For those managing voltage drop in long circuits, we provide a helpful voltage drop calculator and related formulas to ensure system efficiency.

 

Faraday

The Faraday (also known as the Faraday constant) is used in the study of electrochemical reactions and represents the amount of electric charge that liberates one gram equivalent of any ion from an electrolytic solution. It was named in honour of the 19th-century English scientist Michael Faraday and equals 6.02214179 × 10^23 coulombs, or 1.60217662 × 10^-19 electrons.

 

Henry

The henry is a unit of either self-inductance or mutual inductance, abbreviated h (or hy), and named for the American physicist Joseph Henry. One henry is the value of self-inductance in a closed circuit or coil in which one volt is produced by a variation of the inducing current of one ampere per second. One henry is also the value of the mutual inductance of two coils arranged such that an electromotive force of one volt is induced in one if the current in the other is changing at a rate of one ampere per second.

 

Ohm

The unit of resistance in the metre-kilogram-second system is the ohm, named in honour of the 19th-century German physicist Georg Simon Ohm. It is equal to the resistance of a circuit in which a potential difference of one volt produces a current of one ampere (1 ohm = 1 V/A); or, the resistance in which one watt of power is dissipated when one ampere flows through it. Ohm's law states that resistance equals the ratio of the potential difference to current, and the ohm, volt, and ampere are the respective fundamental electrical units used universally for expressing quantities. Impedance, the apparent resistance to an alternating current, and reactance, the part of impedance resulting from capacitance or inductance, are circuit characteristics that are measured in ohms. The acoustic ohm and the mechanical ohm are analogous units sometimes used in the study of acoustic and mechanical systems, respectively. Resistance, measured in ohms, determines how much a circuit resists current, as explained in our page on Ohm’s Law.

 

Siemens

The siemens (S) is the unit of conductance. In the case of direct current (DC), the conductance in siemens is the reciprocal of the resistance in ohms (S = amperes per volt); in the case of alternating current (AC), it is the reciprocal of the impedance in ohms. A former term for the reciprocal of the ohm is the mho (ohm spelled backward). It is disputed whether Siemens was named after the German-born engineer-inventor Sir William Siemens(1823-83) or his brother, the engineer Werner von Siemens (1816-92).

 

Volt

The unit of electrical potential, potential difference, and electromotive force in the metre—kilogram—second system (SI) is the volt; it is equal to the difference in potential between two points in a conductor carrying one ampere of current when the power dissipated between the points is one watt. An equivalent is the potential difference across a resistance of one ohm when one ampere of current flows through it. The volt is named in honour of the I8th—I9th-century Italian physicist Alessandro Volta. Ohm's law defines these electrical units, where resistance equals the ratio of potential to current, and the respective units of ohm, volt, and ampere are used universally for expressing electrical quantities. Energy consumption is measured in kWh, or kilowatt-hours. Explore how devices like ammeters and voltmeters are used to measure current and voltage across components. To better understand how voltage is measured and expressed in volts, see our guide on what is voltage.

 

Watt

The watt is the unit of power in the SI equal to one joule of work performed per second, or to 1/746 horsepower. An equivalent is the power dissipated in a conductor carrying one ampere of current between points at a one-volt potential difference. It is named in honour of James Watt, British engineer and inventor. One thousand watts equals one kilowatt. Most electrical devices are rated in watts. Learn how a watt defines power in electrical systems and its relationship to volts and amperes through Watts' Law.

 

Weber

The weber is the unit of magnetic flux in the SI, defined as the amount of flux that, linking a circuit of one turn (one loop of wire), produces in it an electromotive force of one volt as the flux is reduced to zero at a uniform rate in one second. It was named in honour of the 19th-century German physicist Wilhelm Eduard Weber and equals 10 to the 8th maxwells, the unit used in the centimetre—gram—second system.

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Capacitors Explained

Capacitors store electrical energy via a dielectric, offering capacitance for filtering, smoothing, and decoupling in AC/DC circuits, RC networks, and power supplies, spanning ceramic, film, and electrolytic types with distinct impedance profiles.

 

What Are Capacitors?

Capacitors store charge using a dielectric, providing capacitance for filtering, timing, and decoupling in circuits.

✅ Types: ceramic, film, tantalum, electrolytic; surface-mount or through-hole

✅ Functions: decoupling, bulk energy storage, timing, AC coupling

✅ Key specs: capacitance, voltage rating, ESR/ESL, tolerance, ripple

 

Capacitors for Power Factor Correction

It is desirable to add shunt capacitors in the load area to supply the lagging component of current with a positive negative charging electrons. The cost is frequently justified by the value of circuit and substation capacity released and/or reduction in losses. Installed cost of shunt capacitors is usually least on primary distribution systems and in distribution substations. For foundational context, see what a capacitor is to understand reactive power roles.

The application of shunt capacitors to a distribution feeder produces a uniform voltage boost per unit of length of line, out to its point of application. Therefore, it should be located as far out on the distribution system as practical, close to the loads requiring the kilovars. There are some cases, particularly in underground distribution, where secondary capacitors are economically justified despite their higher cost per kilovar. The placement effectiveness also depends on capacitance characteristics relative to feeder impedance.

Development of low-cost switching equipment for capacitors has made it possible to correct the power factor to a high value during peak-load conditions without overcorrection during light-load periods. This makes it possible for switched capacitors to be used for supplementary voltage control. Time clocks, temperature, electric charge voltage, current flows, and kilovar controls are common actuators for high frequency capacitor switching. Utilities typically choose among several types of capacitors to balance switching duty and reliability.

Capacitor Installations

Capacitors for primary systems are available in 50- to 300-kvar single phase units suitable for pole mounting in banks of 3 to 12 units. Capacitors should be connected to the system through fuses so that a capacitor failure will not jeopardize system reliability or result in violent case rupture. When voltage ratings limit a single unit, engineers connect capacitors in series to distribute stress effectively.

 

Effect of Shunt Capacitors on Voltage

Proposed permanently connected capacitor applications should be checked to make sure that the voltage to some customers will not rise too high during light-load periods. Switched capacitor applications should be checked to determine that switching the capacitor bank on or off will not cause objectionable flicker in electronics. Selecting appropriate sizes in the standard unit of capacitance helps manage voltage rise and flicker.

 

Effect of Shunt Capacitors on Losses

The maximum loss reduction on a feeder with distributed load is obtained by locating positively negatively capacitor banks on the feeder where the capacitor kilovars is equal to twice the load kilovars beyond the point of installation. This principle holds whether one or more than one capacitor bank is applied to a feeder. To meet kvar targets with modular banks, utilities often add capacitance in parallel so reactive output scales predictably.

Capacitor kilovars up to 70% of the total kiovar load on the feeder can be applied as one bank with little sacrifice in the maximum feeder-loss discharge reduction possible with several capacitor banks.

A rule of thumb for locating a single capacitor bank on a feeder with uniformly distributed loads is that the maximum loss reduction can be obtained when the capacitor kilovars of the bank is equal to two-thirds of the kilovar load on the feeder. This bank should be located two-thirds of the distance out on the distributed feeder portion for object charging. Deviation of the capacitor bank location from the point of maximum loss reduction by as much as 10 per cent of the total feeder length does not appreciably affect the loss benefit. Therefore, in practice, in order to make the most out of the capacitor's loss reduction and voltage benefits, it is best to apply the capacitor bank just beyond the optimum loss-reduction location.

Batteries and capacitors seem similar as they both store and release electrical energy. However, there are crucial differences between them that impact their potential electronic applications due to how they function differently, depending on insulator material.

 

Supercapacitors

A capacitor battery aligns the molecules of a dielectric across an electric field to store energy. A supercapacitor aligns the charging of an electrolyte on either side of an insulator to store a double-layer charge.

Electrolytic capacitors consist of two or more conductive capacitors plate, separated by a dielectric. When an electric current enters the capacitor, the dielectric stops the flow and a charge builds up and is stored in an electric field between the metallic plates. Each capacitor is designed to have a particular capacitance (energy storage). When a capacitor is connected to an external circuit, a current will rapidly discharge. Plate area, separation, and dielectric constant together determine capacitance and thus energy density.

In a supercapacitor, there is no dielectric between conducting plates; rather, there is an electrolyte and a thin insulator such as cardboard or paper. When a current is introduced to the supercapacitor, ions build on either side of the insulator to generate a double layer of charge, no matter the capacitor charged. Supercapacitors are limited to low voltages, but very high capacitance frequencies, as a high voltage would break down the electrolyte. 

 

Batteries

There are different types of capacitor batteries, which detemine the capacitance of a capacitor. Different battery types are distinguished by their chemical makeup. The chemical unit, called the cell, contains three main parts; a positive terminal called the cathode, negative terminal called the anode, and the electrolyte. Batteries store electric energy. The battery charges and discharges through a chemical reaction that generates a voltage. The store of charge in the battery is able to provide a consistent DC voltage. In rechargeable batteries, the chemical energy that is converted into electricity can be reversed using an outside electrical energy to restore the charge of capacitors storing power in the batteries.

 

 

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Free Electricity Explained

Free electricity is power generated without fuel costs, typically from solar or wind sources. After setup, systems like solar panels can reduce or eliminate bills through net metering, helping promote sustainability and energy independence for homes and businesses.

 

What is Free Electricity?

Free electricity refers to energy that costs nothing to generate after initial setup, typically utilizing natural sources.

✅ Harnesses renewable energy sources like solar panels and wind turbines

✅ Reduces or eliminates long-term electricity costs

✅ Promotes sustainable and eco-friendly living solutions

 

The Reality of Free Electricity

True “free electricity” does not exist in the sense of unlimited, no-cost power available without investment. However, generating your electricity at home through solar panels or small wind systems can reduce your reliance on the power grid and lower your energy bills significantly, sometimes to zero. This cost reduction is what many people mean when they refer to "free electricity."

Purchasing and installing a solar power system is not free, but it pays off over time. It’s a long-term investment that benefits both the environment and your finances. Some homeowners even reach the point where their solar systems generate more electricity than they use.

In such cases, through a policy known as net metering, these homeowners can send excess electricity back to the power grid and receive compensation from their utility company.

 

What is Net Metering?

Net metering is a billing arrangement that allows consumers who generate their own electricity to send excess power back to the grid and receive credit for it. Here’s how it works:

  • Net metering allows you to sell the electricity produced by a solar system on your home back to the electric power grid.

  • Net Metering occurs when your meter spins backwards as solar electricity is being produced, storing the excess energy on the grid.

  • Once energy is actually being consumed, your meter spins forward to collect the energy that has been saved on your electric power grid.

  • For the energy that you do not consume, the electric utility will compensate you. If you get paid enough money from the electricity that you don't use and sell to them, then that profit can be used to pay for your existing consumption, making it essentially free electricity.

Some utilities offer cash payments for the surplus, while others provide energy credits that reduce your bill. Either way, your electricity costs can be significantly reduced—and in some cases, essentially eliminated.

 

Key Considerations for a Free Electricity System

A few things to watch out for when choosing to invest in a Free Electricity solar power system.

  • You must conserve your energy consumption to ensure that you don't exceed the amount of solar energy produced.

  • By exceeding the amount of power generated many times for the grid or saved, you are then charged regular rates for electricity provided by your electric utility.

  • You must watch your solar energy production. Keep track of the daily energy production of your system.

  • Check your utility bill each month to ensure that you are credited or reimbursed for any and all extra energy generated.

  • To control your electricity usage, consider using a time-of-use electric meter to further capitalize on your investment.

 

Utility Policies Vary

Not all utility companies offer generous net metering. Some may only provide energy credits, while others pay wholesale rates for your excess electricity. It's essential to check with your local utility to understand how they handle customer-generated power.

While the term “free electricity” is somewhat misleading, it does accurately reflect the very real possibility of generating low-cost or no-cost power after your initial system is installed. Through renewable energy systems and programs like net metering, homeowners can reduce or eliminate energy bills and make a lasting contribution to a cleaner, more sustainable future.

 

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Electricity Cost Principles Explained

Electricity cost reflects kWh rates, tariffs, demand charges, power factor penalties, and TOU peak/off-peak pricing, driven by load profiles, utility billing, transmission and distribution fees, and efficiency measures in industrial, commercial, and residential systems.

 

What Is Electricity Cost?

Electricity cost is the total price per kWh including energy, demand, and network charges under applicable tariffs.

✅ Includes energy (kWh), demand (kW), and fixed charges

✅ Varies by TOU tariffs, peak/off-peak, and seasons

✅ Affected by power factor, load profile, and efficiency

 

Electricity Cost principles involve looking at how much electricity consumption and we have to understand how it's measured.

At its core, understanding power use starts with grasping what electricity is and how it behaves in circuits.

It is determined at any moment and is measured in watts consumed. For example: if you want to determine the bill energy or bill electricity rate: For a refresher, see what a watt represents to relate device ratings to instantaneous power.

  • A 100-watt light bulb uses 100 watts.
  • A typical desktop computer uses 65 watts.
  • A central air conditioner uses about 3500 watts.

These device ratings illustrate electric load in practical terms as each appliance contributes to total demand.

If you want to know how to rate electricity pricing, you want to know how much energy you're using. When you use 1000 watts for an hour, that's a kilowatt-hour. For example:

  • Ten 100-watt light bulbs on for an hour, is 1 kWh
  • Ten 100-watt light bulbs on for 1/2 an hour, is 0.5 kWh
  • Ten 50-watt light bulbs on for an hour, is 0.5 kWh
  • One 60-watt light bulb on for an hour, is 0.06 kWh (60/1000)
  • Running a 3500-watt air conditioner for an hour is 3.5 kWh.

The average U.S. household used 10,654 kWh a year in 2001, or 888 kWh/mo. (Dept. of Energy) The U.S. as a whole used 3,883 billion kWh in 2003, or 13,868 kwH per person based on a population of 300 million. (Dept. of Energy)

 

Watt-hours

For smaller items we use the term watt-hours instead of kilowatt-hours. For example, we say a 60-watt light bulb uses 60 watt-hours of electricity billed, not 0.060 kWh. If you're unsure, this overview of what a watt-hour means clarifies the relationship between power and time.

Note that the "-hours" part is important. Without it we'd have no idea what period of time we were talking about.

If you ever see a reference without the amount of time specified, it's almost certainly per hour.

If your device lists amps instead of watts, then just multiply the amps times the voltage to get the watts. For example:

2.5 amps x 120 volts = 300 watts

Trivia: On a peak day in 2009, California used 50,743 megawatt-hours of electricity, or 50,743,000,000 watt-hours.

How much does electricity cost?

 

Electricity Cost

It depends on where you live (like Ontario), how much you use, and possibly when you use it. There are also fixed charges that you pay every month no matter how much electricity you use. For example, I pay $6/mo. for the privilege of being a customer of the electric company, no matter how much energy I use. Local infrastructure and electricity supply conditions can also influence pricing tiers.

Check your utility bill for the rates in your area. If it's not on your bill then look it up on the utility's website. National summaries of electricity prices help you compare trends across regions.

The electric company measures how much electricity you use in kilowatt-hours. The abbreviation for killowatt-hour is kWh. Note that on your bill there can be multiple charges per kWh (e.g., one for the "base rate", another for "fuel") and you have to add them all up to get the total cost per kWh. This measurement is recorded by a watt-hour meter that cumulatively tracks energy over time.

Most utility companies charge a higher rate when you use more than a certain amount of energy, and they also charge more during summer months when electric use is higher. As an example, here are the residential rates prices electricity for Austin, Texas (as of 11-03):

First 500 kilowatts5.8¢ per kilowatt hour (kWh)

Additional kilowatts (May-Oct.)10¢ per kilowatt hour

Additonal kilowatts (Nov.-Apr.)8.3¢ per kilowatt hour

These figures include a fuel charge of 2.265¢ per kWh.

The average cost of residential electricity was 9.86¢/kWh in the U.S. in March 2006. The average household used 888 kWh/mo. in 2001 and would pay $87.56 for it based on the March 2006 average rate. (Dept. of Energy)

The cost of electricity varies by region. In 2003 the price ranged from 5.81¢ in Tennessee to 12¢ in California, 14.314¢ in New York, and 16.734¢ in Hawaii. In Summer 2001, electricity was a whopping 20¢/kWh in parts of California.

 

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