Electromagnetism and Magnetomotive Force Quiz
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Questions and Answers

What is the formula for calculating the magnetomotive force (MMF)?

𝛩 = 𝐼 ∙ 𝑤

Explain the relationship between the current (I) and the magnetomotive force (MMF) in a solenoid.

The magnetomotive force (MMF) is directly proportional to the current (I) flowing through the solenoid. Therefore, increasing the current will increase the MMF, and vice versa.

What is the effect of increasing the number of windings (w) in a solenoid on the magnetomotive force (MMF)?

Increasing the number of windings (w) in a solenoid will also increase the magnetomotive force (MMF).

Explain why the MMF generated by three individual coils with one winding each carrying current I is the same as the MMF generated by one coil with three windings carrying the same current I.

<p>The MMF is determined by the total number of ampere-turns, which is the product of current (I) and the number of windings (w). In both cases, the total number of ampere-turns is the same, so the MMF is equal.</p> Signup and view all the answers

What are the two main factors that influence the magnetomotive force (MMF) of a solenoid?

<p>The two main factors that influence the MMF of a solenoid are the current (I) flowing through the coil and the number of windings (w) in the coil.</p> Signup and view all the answers

Explain the concept of magnetic monopoles and why they are believed not to exist.

<p>Magnetic monopoles are hypothetical particles that have only a north or south magnetic pole, whereas all known magnets have both a north and south pole. The current understanding is that magnetic fields always exist as closed loops, not originating or ending at a single point, making the existence of magnetic monopoles unlikely.</p> Signup and view all the answers

What is the significance of the equation ර 𝐵 ∙ 𝑑 𝑠Ԧ = 0 as related to the magnetic field?

<p>This equation, known as Gauss's Law for magnetism, implies that the magnetic flux through any closed surface is zero. It means that magnetic field lines form closed loops and do not originate or terminate at any point, supporting the absence of magnetic monopoles.</p> Signup and view all the answers

Why is the statement "magnetic field lines never cross" significant?

<p>Magnetic fields are vector quantities, meaning they have both magnitude and direction. If the fields from multiple magnets overlap, their directions are added vectorially to create a single combined magnetic field strength at that point. Therefore, magnetic field lines cannot cross because they would be representing two different directions at the same point, which is not physically possible.</p> Signup and view all the answers

Describe the direction of the magnetic field lines inside a bar magnet.

<p>The magnetic field lines inside a bar magnet run from the south pole to the north pole, forming continuous loops.</p> Signup and view all the answers

What is the relationship between magnetic flux and magnetic field strength?

<p>Magnetic flux is the measure of the total magnetic field passing through a given area. It is proportional to the magnetic field strength and the area of the surface.</p> Signup and view all the answers

How is the combined magnetic field determined when two or more magnetic fields overlap?

<p>The combined magnetic field is determined through vector addition of the individual magnetic fields at each point where they overlap.</p> Signup and view all the answers

What is the significance of the statement: "The magnetic field lines do not originate and terminate on poles – they form closed loops."?

<p>This statement emphasizes the absence of magnetic monopoles and the fundamental nature of magnetic fields as continuous, closed loops that do not begin or end at any singular points.</p> Signup and view all the answers

What is the role of the magnetic field in an electric circuit?

<p>The magnetic field plays a crucial role in electromagnetic induction, where changing magnetic fields induce electric currents, a fundamental principle in transformers, generators, and motors.</p> Signup and view all the answers

What is the primary factor that leads to winding losses in a transformer?

<p>The resistivity of the material used for the windings.</p> Signup and view all the answers

Why is reducing current flow not a practical solution to minimize winding losses in a transformer?

<p>Because current flow is determined by the load requirements.</p> Signup and view all the answers

Explain the main difference between core-type and shell-type transformer arrangements.

<p>In core-type transformers, the windings surround the core, while in shell-type transformers, the core surrounds the windings.</p> Signup and view all the answers

Why is it important to minimize winding losses in transformers?

<p>Minimizing losses increases efficiency and reduces energy waste.</p> Signup and view all the answers

What are two primary materials used for transformer windings, and why are they preferred?

<p>Copper and aluminum are preferred for their low resistance and cost-effectiveness.</p> Signup and view all the answers

Describe the relationship between the low voltage winding and the high voltage winding in both core-type and shell-type transformers.

<p>The low voltage winding is wound directly on the core, and the high voltage winding is wound over it in both types of transformers.</p> Signup and view all the answers

What is one key advantage of using a shell-type transformer arrangement?

<p>Shell-type transformers offer better magnetic flux containment, reducing external magnetic fields compared to core-type transformers.</p> Signup and view all the answers

Why is it important to consider the cost implications when selecting materials for transformer windings?

<p>Balancing performance with cost factors is crucial for ensuring the economic viability of transformer design and production.</p> Signup and view all the answers

Explain the relationship between inductance and the rate of current change in a circuit.

<p>Inductance (L) is a measure of an inductor's opposition to changes in current. The larger the inductance, the greater the induced voltage for a given rate of current change.</p> Signup and view all the answers

What is mutual inductance and how does it relate to the coupling between two coils?

<p>Mutual inductance (M) is the property of two coils where a changing current in one coil induces a voltage in the other coil. Higher mutual inductance means that the magnetic flux from the first coil is more effectively linked to the second coil, resulting in a stronger coupling between them.</p> Signup and view all the answers

Describe how the induced voltage in the second coil is determined in a system with mutual inductance, and how it relates to the changing current in the first coil.

<p>The induced voltage in the second coil (ε2) is proportional to the rate of change of the magnetic flux (𝛷12) that is linked to the second coil. Since this flux is generated by the changing current in the first coil, the induced voltage in the second coil is ultimately determined by the rate of change of current (di1/dt) in the first coil and the mutual inductance (M) between the two coils.</p> Signup and view all the answers

What is the formula for the coupling inductance (M) between two coils and what does it represent in terms of the individual inductances of each coil?

<p>The coupling inductance (M) is calculated as the square root of the product of the individual inductances (L1 and L2) of the two coils: M = √(L1 * L2). This formula represents the strength of the magnetic coupling between the coils. A higher mutual inductance indicates tighter coupling, meaning more of the magnetic field from one coil links to the other.</p> Signup and view all the answers

How is the induced voltage in the second coil related to the mutual inductance and the rate of change of current in the first coil? Write the formula.

<p>The induced voltage in the second coil (ε2) is directly proportional to the mutual inductance (M) and the rate of change of current (di1/dt) in the first coil. This can be expressed by the formula: ε2(t) = -M12 * (di1(t)/dt).</p> Signup and view all the answers

What is the practical significance of mutual inductance in the design of transformers?

<p>Mutual inductance plays a critical role in the operation of transformers. It allows the transfer of electrical energy between the primary and secondary coils without any direct connection. By designing the coils to have a high mutual inductance, a significant portion of the magnetic field generated by the primary coil links to the secondary coil, ensuring efficient energy transfer. This principle is fundamental to the operation of electrical power grids and numerous other electrical applications.</p> Signup and view all the answers

Explain the relationship between flux linkage and mutual inductance. How does the choice of materials surrounding the coils affect the flux linkage and mutual inductance?

<p>Flux linkage refers to the amount of magnetic flux that passes through one coil due to the magnetic field generated by another coil. Mutual inductance is directly proportional to this flux linkage. Materials surrounding the coils can significantly alter the flux linkage and hence the mutual inductance. For instance, materials with high permeability, like iron, will concentrate the magnetic flux, leading to increased flux linkage and a higher mutual inductance. Conversely, materials with low permeability will have a weaker magnetic field and lower mutual inductance.</p> Signup and view all the answers

Explain the concept of magnetic induction, and how it relates to the idea of induced voltage in a coil.

<p>Magnetic induction occurs when a changing magnetic field induces an electromotive force (emf) within a conductor. This induced emf drives the flow of current in the conductor. In a coil, the changing magnetic field can be generated either by the changing current within the coil itself (self-induction) or by the changing current in a nearby coil (mutual induction). When the magnetic field changes, the induced voltage is proportional to the rate of change of the magnetic flux through the coil. This phenomenon is the foundation for many electrical devices like generators and transformers.</p> Signup and view all the answers

Under what condition does a transformer's secondary voltage become zero? Explain why this happens.

<p>A transformer's secondary voltage becomes zero during a short circuit. This occurs because the short circuit creates a low resistance path, causing a large current to flow through the secondary winding. The high current leads to a significant voltage drop across the internal impedance of the transformer, effectively reducing the secondary voltage to zero.</p> Signup and view all the answers

What is the significance of the short-circuit voltage in a transformer? Why is it an important consideration during parallel operation of transformers?

<p>The short-circuit voltage is crucial in assessing the ability of a transformer to withstand fault conditions and is a major factor in transformer performance. It's essential during parallel operations to ensure transformers have compatible short-circuit voltage ratings. This prevents a large current imbalance between them during a fault, potentially causing damage to the system.</p> Signup and view all the answers

What are the three key factors that contribute to non-ideal behavior in a single-phase transformer?

<p>The three key factors are core losses, winding losses (in both the primary and secondary), and flux leakage.</p> Signup and view all the answers

Why can the core resistance (𝑅𝐶) and the main inductive reactance (𝑋1𝜇) be neglected during short-circuit conditions in a transformer?

<p>Under short-circuit conditions, the core resistance and main inductive reactance are typically much smaller in magnitude compared to the other resistances and leakage reactances in the circuit. Therefore, their contribution to the overall impedance is negligible and can be disregarded for simplifying analysis.</p> Signup and view all the answers

Explain the concept of 'short-circuit equivalent circuit' and why it's useful for describing the behavior of a transformer under typical load conditions.

<p>The short-circuit equivalent circuit represents the transformer's behavior under short-circuit conditions, taking into account all resistances and reactances. It is especially useful for analyzing the transformer's performance at loads greater than 30% of its rated power. This is because under typical loads, the transformer's magnetic saturation effects are less pronounced, and the equivalent circuit effectively captures the key impedance characteristics.</p> Signup and view all the answers

Describe the conditions under which core losses are measured in a single-phase transformer.

<p>Core losses are measured under open-circuit conditions, meaning no load is connected to the secondary winding.</p> Signup and view all the answers

What are the factors that influence the short-circuit behavior of a transformer?

<p>The short-circuit behavior of a transformer is primarily influenced by the internal resistances (𝑅1 and 𝑅2') and leakage reactances (𝑋1𝜎 and 𝑋2𝜎) within the transformer windings. These factors directly impact the impedance of the circuit and determine the amount of current flowing during a fault.</p> Signup and view all the answers

What is the primary function of the current flowing in the primary winding of a single-phase transformer during the open-circuit condition?

<p>The primary current compensates for core losses (resistive part) and provides the magnetizing current (reactive part) required to establish the magnetic field in the core.</p> Signup and view all the answers

What is the role of the 'short-circuit equivalent circuit' in understanding the behavior of a transformer under various load conditions?

<p>The short-circuit equivalent circuit simplifies the analysis of a transformer by representing its internal impedances (resistances and reactances). Its usefulness lies in providing a tool for understanding the transformer's performance under different load conditions, from light loads to heavy loads, without needing to analyze the complex magnetic circuit of the core.</p> Signup and view all the answers

Explain why flux leakage is a factor that contributes to non-ideal behavior in a transformer.

<p>Flux leakage occurs when a portion of the magnetic flux generated by the primary winding does not link the secondary winding, which reduces the efficiency of energy transfer between the windings.</p> Signup and view all the answers

Why is it important to understand the short-circuit behavior of a transformer in a power system?

<p>Understanding the short-circuit behavior of a transformer is critical for designing and operating power systems safely. This knowledge helps to ensure the stability of the system, prevent damage to equipment during faults, and design protective devices to isolate and clear faults promptly.</p> Signup and view all the answers

What is the significance of the open-circuit test in evaluating the performance of a single-phase transformer?

<p>The open-circuit test allows for the measurement of core losses, which are primarily caused by hysteresis and eddy currents within the transformer's core.</p> Signup and view all the answers

Explain how the short-circuit voltage of a transformer is related to its ability to withstand short-circuit currents.

<p>The short-circuit voltage is directly related to the transformer's ability to withstand short-circuit currents. A lower short-circuit voltage indicates a higher internal impedance, which helps to limit the current flow during a fault. Higher impedances are more desirable in transformer design, as they offer better protection against damage from short circuits.</p> Signup and view all the answers

Explain the mechanism by which core losses manifest in a transformer.

<p>Core losses arise primarily due to hysteresis loss, caused by the magnetization and demagnetization of the core material, and eddy current loss, caused by circulating currents induced in the core by the changing magnetic field.</p> Signup and view all the answers

How do core losses impact the overall efficiency of a single-phase transformer?

<p>Core losses, being resistive in nature, consume power without contributing to the output power of the transformer. This reduces the overall efficiency, meaning that not all the input power is transferred to the load.</p> Signup and view all the answers

Explain the significance of winding losses in the context of a non-ideal single-phase transformer.

<p>Winding losses, primarily due to the resistance of the primary and secondary windings, result in a voltage drop within the windings, reducing the voltage available to the load and decreasing energy transfer efficiency.</p> Signup and view all the answers

Flashcards

Magnetic Monopoles

Hypothetical particles that would carry a single magnetic pole, not observed in nature.

Magnetic Field

A region around a magnet where magnetic forces are exerted, represented by lines.

Closed Loops

Magnetic field lines form complete loops, never starting or ending on the poles.

Induction

The process by which a changing magnetic field creates an electric current.

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Magnetizing Force

The force that magnetizes a material to align its magnetic domains.

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Non-Ideal Transformer

A transformer that does not operate at 100% efficiency due to losses.

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Ideal Transformer

A theoretical transformer that has no losses and perfectly transfers energy.

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Vector Addition of Magnetic Fields

When magnetic fields from different sources overlap, they add as vectors to form a single field.

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Magnetomotive Force (MMF)

The driving force in a magnetic circuit, calculated as MMF = I × w, where I is current and w is the number of windings.

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Current (I)

The flow of electric charge through a conductor, measured in Amperes (A).

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Windings (w)

The number of loops or turns in a coil, which affects the generation of a magnetic field.

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Solenoid

A coil of wire designed to create a magnetic field when an electric current passes through it.

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Relationship of MMF to windings and current

Increasing either the current or the number of windings increases the magnetomotive force, generating a stronger magnetic field.

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Inductance (L)

The measure of an inductor’s response to current change, in Henries.

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Mutual Inductance

When a change in current in one coil induces voltage in another coil.

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Magnetic Flux (Φ)

The total magnetic field passing through a given area.

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Induced Voltage (ε₂)

Voltage produced in a coil due to a changing magnetic flux.

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Coupling Inductance (M₁₂)

The inductance between two coils, calculated as L₁*L₂.

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Rate of Change of Current

How quickly the current is changing over time.

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Coil 1 (i₁)

First coil in a mutual induction setup whose current creates magnetic flux.

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Coil 2 (i₂)

Second coil that experiences induced voltage due to the flux from Coil 1.

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Winding Losses

Energy lost due to the resistivity of winding materials, resulting in heating.

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Copper Losses

Power losses in a transformer due to the resistance of copper windings when current flows.

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I²R Losses

Loss of power in a conductor due to its resistance and the square of the current flowing through it.

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Transformer Winding Resistance

The inherent resistance in transformer windings that causes energy loss during operation.

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Core-Type Transformer

A transformer design where windings surround a magnetic core for efficient flux use.

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Shell-Type Transformer

A design where the magnetic core encases the windings, optimizing magnetic paths.

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Low Resistance Materials

Materials like copper or aluminum used in transformers to minimize energy losses.

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Magnetizing Current Losses

Energy losses in a transformer even without load, due to resistance to magnetizing current.

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Core Losses

Energy losses in a transformer due to hysteresis and eddy currents in the core.

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Primary Winding

The winding in a transformer connected to the input voltage source.

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Secondary Winding

The winding in a transformer connected to the output load where transformed voltage is delivered.

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Flux Leakage

The magnetic flux that does not link both primary and secondary windings in a transformer.

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Induction in Transformers

The process by which a changing magnetic field in the primary winding creates a voltage in the secondary winding.

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Magnetizing Current

The current that establishes the magnetic field in the transformer core when it's energized but not delivering power.

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Open-Circuit Condition

A condition when the primary winding is energized, but there's no load connected to the secondary winding.

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Short Circuit

A condition where the secondary voltage is zero due to a direct connection in the circuit.

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Short Circuit Voltage

The voltage across the transformer during a short circuit, crucial for performance evaluation.

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Core Resistance (RC)

Resistance in the transformer's core, plays a role in short circuit behavior.

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Inductive Reactance (X1μ)

The main inductive reactance of a transformer, significant in evaluating short circuits.

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Equivalent Circuit

A simplified electrical circuit representation during short circuit conditions, typically used above 30% load.

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Transformers in Parallel

Multiple transformers working together, their short-circuit voltage is crucial for efficiency.

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Secondary Current (I2SC)

The current in the secondary circuit during a short circuit condition.

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Short Circuit Behavior

Refers to how transformers perform under short circuit conditions, including losses.

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Study Notes

Fundamentals of Electrical Engineering - Lecture 7: Transformer

  • The lecture covers transformers, magnetism, and materials.
  • The lecture is presented by Prof. Dr.-Ing. Saša Bukvić-Schäfer (Hochschule Hamm-Lippstadt) and Prof. Dipl.-Ing. Volker Wachenfeld (Hochschule Biberach).
  • The date of the lecture is 04.12.2024.

Agenda

  • Fundamentals - Electromagnetism:
    • Magnetic field
    • Magnetizing force and magnetic induction
    • Induction
  • Transformer:
    • Ideal single-phase transformer
    • Non-ideal single-phase transformer
    • Three-phase transformer

Basic Concepts: Magnets

  • Magnets have a long history (thousands of years) and have been mainly used as compasses.
  • To describe magnets, you must accept that magnets cannot have only a north or south pole; they always come in pairs.
  • No magnetic monopoles exist

Basic Concept: Magnetic Field

  • Magnetic field: no sources or sinks - Maxwell: ∮B • ds = 0!
  • The magnetic field lines do not originate and terminate on poles – they form closed loops.
  • Although magnetic field lines appear to originate at the north pole and terminate on the south pole, they run within the magnet between the poles.
  • Magnetic field lines never cross. If fields from two or more magnets overlap, the fields add vectorially to produce a single, total field at that point.
  • The net magnetic field at any point is the vector sum of all magnetic field lines present at that point.
  • Magnetism and electricity are interdependent.
  • Experimental work by Ørsted (1820) showed that a magnetic needle is deflected by an adjacent electric current and aligns itself perpendicularly to a current-carrying wire.
  • Ampère extended the work of Örsted and developed a mathematical and physical theory to understand the relationship between electricity and magnetism.
  • For any closed loop path, the sum of the length elements times the magnetic field strength in the direction of the length element is equal to the all electric current enclosed in the loop (H • ds = ∮ Ienc ).

Basic Concept: Magnetic Field - Ampère

  • For a closed loop path the sum of the length elements times the magnetic field strength (H) in the direction of the length element is equal to all electric current enclosed in the loop.
  • Ampère demonstrated that current through a conductor will create a circular magnetic field around it.
  • The line integral of the magnetic field around the conductor equals the current through it (H • ds = Ienc ).

Fundamentals of Electromagnetism – Magnetic Parameters

  • Cause? Voltage(V).
  • Effect? Current(I).
  • Direction?
  • I = V/R

Fundamentals of Electromagnetism – Magnetic Parameters

  • Cause = "driving" parameter depending on Current.
  • Idea: The current is conducted as an effect of the voltage (Ohm's law). The voltage itself has no direct impact on the magnetic field.

Fundamentals of Electromagnetism – Magnetic Parameters

  • Cause(driving parameter): Current and Number of windings of the solenoid (= coil).
  • Magnetic parameter: Magnetomotive Force! Θ = I • w

Fundamentals of Electromagnetism – Magnetic Parameters

  • Magnetic flux φ = Sum of all field lines penetrating the cross section S.
  • φ = w • I

Fundamentals of Electromagnetism – Magnetic Parameters

  • Magnetic parameter: Magnetomotive Force!
  • Effect = Field inside the solenoid depending cause (magnetomotive force) and material properties.
  • Magnetic parameter: Magnetic flux! φ = φ • Rm

Fundamentals of Electromagnetism – Electrical Equivalent Circuit

  • Magnitude of the magnetic flux depends on conductivity of the material, length of the field lines, and cross-section.
  • Greater the reluctance (magnetic resistance), the greater the resistance of the magnetic flux.

Induction - Faraday’s Law

  • AC power generation is based on Faraday’s Law of induction.
  • The induced electromotive force in any closed circuit is equal to the negative of the time rate of change of the magnetic flux enclosed by the circuit.
  • ε = v(t) = - w • dΦ(t)/dt

Induction - Faraday's Law

  • Factors influencing the induced electromotive force (EMF, ε) or voltage:
    • The number of windings in the coil
    • The speed of the relative motion between the coil and the magnet
    • The strength of the magnetic field

Induction - Lenz’s Law

  • If a magnetic field induces a voltage in a conductor, the direction of the induced current will be to minimize the change in magnetic flux. (Think of inertia, opposing the change in velocity)

Self Inductance

  • Due to the change in magnetic flux, voltage is induced as a result of the change in the inducing current.
  • Flux change due to current change
  • ε = -w • d(w • i(t)/Rm)/dt
  • ε = -w² • μ₀ • μᵣ • S • di(t)/dt
  • Inductance L is the property of a component that opposes any change in current flowing through it.

Inductance

  • Inductance (L): L = w² • μr • μo • l/S
  • Geometry: S = π • D²/4
  • Where:
    • w = Number of windings
    • μr = permeability of the core material
    • μo = permeability of vacuum
    • l = Length of the solenoid
    • D = Diameter of the solenoid
  • The basic unit of measurement for inductance is the Henry [H]. A circuit has an inductance of one Henry when an emf of one volt is induced in the circuit and the current flowing through it changes at a rate of one ampere/second.

Mutual Inductance

  • Current i₁ (t) “creates” a magnetic flux φ₁
  • The second coil is exposed to the major part of this flux (φ12)
  • The induced voltage in the second coil is dependent on the change of flux seen by the second coil:
    • ε₂(t)= -W₂ • dφ₁₂(t)/dt
  • As the changing flux is a result of changing current in the first coil, the formula can be re-written: ε₂(t)= -M₁₂ • di₁(t)/dt
  • With the coupling inductance M₁₂ = √L₁ L₂.

Transformer

  • A transformer is a static device that changes the alternating voltage form one level to another without changing the frequency.
  • Transformers are important electrical-electrical energy conversion components.
  • One important reason we use AC is because we can easily change the voltage levels.
  • Transformers enable this conversion of voltage level with high efficiency (up to 99%).
  • Transformers have no moving parts (low maintenance).

Transformer Parts

  • A transformer basically consists of two or more windings wrapped around a common core.
  • The primary winding is connected to the AC electric power source.
  • The secondary winding has a desired voltage level and is connected to the load.

Transformer Parts - Magnetic Core

  • The core magnetically couples the windings.
  • The core material should have high permeability ("conductivity" for the flux).
  • Ferromagnetic/ferrite materials are suitable.
  • Hysteresis losses occur each time the magnetic field reverses.

Transformer Parts – Magnetic Core: Hysteresis Losses

  • Classification of soft or hard magnetic materials based on their hysteresis characteristics.
  • Soft magnetic materials are utilized in devices subjected to alternating magnetic fields and in which low energy loss is needed (transformer core).
  • Hard magnetic materials utilized in permanent magnets which must have no resistance to demagnetization.
  • Hysteresis losses: P hyst = Vmaterial • 1/f • ∫H • dB

Transformer Parts – Windings

  • The winding that receives electrical energy (from the source) is called the primary winding.
  • The winding that receives energy from the primary winding, via the magnetic field, is called the secondary winding.
  • Either the high or low voltage winding can be the primary or secondary.

Transformer Parts - Windings

  • There is some loss of energy that is due to the resistance of the windings (primary or secondary) to the magnetizing current, even with no load attached.
  • The loss of electrical energy is increased when the load is applied to the transformer.
  • Loss can be reduced by choosing a conducting material with lower resistance per cross-sectional area. Suitable materials for transformers are Copper and Aluminum.

Transformer Arrangements

  • Core-type: Winding surrounds the core.
  • Shell-type: The core forms a shell surrounding the windings.
  • Both low and high-voltage windings are either wound directly onto the core and or wound over the low-voltage winding.

Ideal Single-Phase Transformer

  • Ideal means no losses.
  • No core losses (Rm,Fe = μ₀ • μr • l/A).
  • Near infinite core permeability (μr → ∞).
  • No eddy currents.
  • No winding resistance (Rcu → 0).
  • No flux leakage (only main magnetic flux Φ12 linking both windings: Φ₁ = Φ₂ = Φ₁₂).

Ideal Single-Phase Transformer

  • Primary coil with w₁ windings
  • Secondary coil with w₂ windings
  • Φ₁₂(t) is generated by the varying current i₁(t) in the primary winding.

Ideal Single-Phase Transformer

  • Same flux passes through both coils: Φ₁(t) = Φ₂(t) = Φ₁₂(t).
  • ν₁(t)/w₁ = ν₂(t)/w₂

Ideal Single-Phase Transformer

  • Now a load R₂ is connected to the secondary coil.
  • A current I₂(t) is delivering power to the load with power p₂ = v₂ . i₂
  • No loss in an ideal transformer.
  • P₁ = v₁ • i₁ = v₂ • i₂ = p₂

Non-Ideal Single-Phase Transformer

  • Non-ideal operation: core losses, winding losses (primary and secondary), flux leakage.

Non-Ideal Single-Phase Transformer - Core Losses

  • Open-circuit condition (no load): Losses are primarily due to core losses (resistive, often represented by Rc).
  • Magnetizing current i₁(t) = im(t) + ic(t) is a phasor sum of the reactive component and resistive part.

Non-Ideal Single-Phase Transformer - Core Losses

  • Voltage V₁ is in-phase with the resistive component and leads the magnetization current (ωt) by 90 degrees.
  • Induced voltage in the secondary winding V₂ will now be under no-load conditions in phase with V₁

Non-Ideal Single-Phase Transformer - Winding Losses

  • The primary winding is supplied by AC voltage creating a magnetic flux φ₁.
  • This magnetic flux φ₁ consists of main flux φ₁₂ and leakage flux φ₁σ
  • The same is true for the secondary side, with φ₂ = φ₁₂ + φ₂σ.

Non-Ideal Single-Phase Transformer - Winding Losses

  • Leakage flux φ₁σ and φ₂σ do not link both windings
  • Voltage is affected by leakage inductance (X₁σ and X₂σ)
  • Equivalent Circuit diagrams take winding and core losses into account.

Equivalent Circuit

  • Primary and secondary sides consist of Resistance(R), Inductance(X) and Core losses(Rc) and Magnetizing Reactive part(Xμ)
  • Secondary side parameters are calculated based on primary side parameters using the ratio w1/w2.

Equivalent Circuit

  • Adding all parts together
  • V₁ = jX₁ • I₁ + I₁ • R₁ + V₁μ
  • V₂ = jX₂ • I₂ + I₂ • R₂ - V₂μ

Open Circuit - No Load Conditions

  • In an open circuit (no load), the secondary current (I₂) is zero.
  • The current in the primary winding, i₁, is only related to magnetizing the core and covering the losses in the core and primary winding (typically, this current I₁0 is very small).

Short Circuit Conditions

  • In short-circuit conditions, the secondary voltage is zero.
  • The core resistances and main inductive reactance are typically much greater than the other resistance and inductive leakage reactances and can be neglected.
  • Short-circuit behavior is an important criterion for transformer performance, especially during parallel operations.

Transformer Under Load Conditions

  • Under typical load conditions, the equivalent circuit can be used to calculate voltages.
  • VR = RT • I₁ and Vx = jXT • I₁
  • The calculated values can be used with Kirchhoff’s law to determine the overall voltage

Three-Phase Transformer

  • Three sets of primary and secondary windings (one per phase). Wound on the same core.
  • Windings can be connected in various ways, such as Y or delta

Three-Phase Y-Connection

  • Three-phase system in a low-voltage grid with symmetrical AC voltage sources (the AC voltage supplies form a common star or middle/wye-connection).
  • The formula for calculating phase voltages (V1, V2, V3), line voltages V12, V23, V31, and neutral current In can be used to calculate three-phase transformer operation.

Transformer Configuration

  • Choice of connection for a three-phase transformer depends on several factors:
    • 3 or 4 wire network.
    • Load asymmetry: think about single-phase and 3-phase loads.
    • Economic reasons: cost of construction and connection method.

Transformer Configuration

  • Consider the difference between Y and Δ connections (star, delta):
    • In a Y connected winding, the current trough each phase winding is the line current divided by √3.
    • In a Δ connected winding, it requires √3 times as many windings as a Y-connected winding for the same voltage.

Single-Phase Equivalent Circuit Diagram of a Three-Phase Transformer

  • In a wye connection the sum of the three currents( I₁ +I₂ + I₃ = 0).
  • For symmetric loads, the neutral conductor can be omitted.

Parallel Operation of Transformers

  • Parallel operation of Transformers is impacted when both the HV and LV windings are connected to the same set of HV and LV busbars.
  • Two impedances in parallel = combined impedance, which is less than either of the components.
  • Care must be taken to ensure that the fault capability of the LV switchgear is not exceeded.

Parallel Operation of Transformers

  • For parallel operation, the same connection symbol, voltage ratio, percentage impedance/short-circuit voltage, and the same phase sequence must be maintained.
  • In perfect parallel operation, current in each transformer is proportional to the transformer capacity, with the total current being the arithmetic sum.

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Test your knowledge on the concepts of magnetomotive force (MMF), including its formula and the effects of current and windings in a solenoid. Explore the significance of magnetic field lines and the factors influencing magnetic flux. This quiz covers key principles of electromagnetism and magnetic theory.

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