Transformer Excitation Current Testing

Protec Equipment Resources
8 Dec 202345:58

Summary

TLDRIn this webinar, Tom Sandry, the director of Workforce Development at Vector Power, dives into the intricacies of transformer excitation current testing. He refreshes participants on magnetism, magnetic induction, and Faraday's and Lenz's laws, setting the stage for a deeper understanding of the test's purpose. Sandry explains how excitation current tests can detect winding and core issues in transformers, even when other tests show normal results. He discusses the physics behind the test, the significance of phase patterns, and how to perform the test with necessary safety precautions. The webinar concludes with a quiz to reinforce the key learnings and a Q&A session, providing a comprehensive guide for professionals in the field.

Takeaways

  • ๐Ÿงฒ The webinar by Tom Sandry from Vector Power focused on Transformer excitation current testing, which is crucial for diagnosing transformer health.
  • ๐Ÿ” Magnetism is foundational to understanding excitation current testing, with magnetic fields, flux, and lines of force being key concepts.
  • ๐Ÿ‘ The left-hand rule helps determine the relationship between current flow and the direction of magnetic lines of force around a conductor.
  • ๐Ÿ“š Magnetic permeability is analogous to electrical conductivity, with high permeability materials concentrating magnetic flux lines effectively.
  • ๐Ÿ”— The relationship between magnetism and electrical current is demonstrated through Ohm's law in the magnetic world, relating MMF, reluctance, and flux.
  • ๐ŸŒ Electromagnetic induction, discovered by Michael Faraday, is the process where a voltage is induced in a conductor that cuts through magnetic field lines.
  • ๐Ÿ‘ฃ Lenz's Law explains the polarity of induced voltage, which opposes the change causing the induction, setting up a magnetic field around the conductor.
  • ๐Ÿš€ The excitation current test is valuable for detecting winding and core problems in transformers, even when other tests seem normal.
  • ๐Ÿ” The test can identify issues like abnormal core grounds, winding faults, low tap changer problems, and manufacturing defects.
  • ๐Ÿ“ˆ Phase patterns in three-phase transformers can indicate potential problems; normal patterns are high-low-high or low-high-low, with deviations suggesting issues.
  • ๐Ÿ› ๏ธ The procedure for performing excitation current tests involves careful setup, safety considerations, and comparison of results to previous tests or benchmarks.

Q & A

  • What is the main focus of the webinar presented by Tom Sandry from Vector Power?

    -The webinar focuses on Transformer excitation current testing, covering topics such as magnetism, magnetic induction, the physics behind the test, and how to identify faults in transformers using this method.

  • Why is a refresher on magnetism important for understanding excitation current testing?

    -A refresher on magnetism is important because the theory behind excitation current testing is deeply rooted in the understanding of magnetic fields, magnetic flux, and the principles of electromagnetism.

  • What is magnetic flux and how is it represented?

    -Magnetic flux is the group or number of magnetic field lines emitted outward from the North Pole of a magnet. It is represented by the symbol 'ฮฆ' (phi), and its SI unit is the Weber.

  • Can you explain the left-hand rule for current-carrying conductors?

    -The left-hand rule helps determine the relationship between the current flow through a conductor and the direction of the magnetic lines of force around it. If you point your thumb in the direction of the positive potential and wrap your fingers around the conductor, your fingers indicate the direction of the magnetic field.

  • How does adding an iron core to a coil affect the magnetic field?

    -Adding an iron core inside a coil increases the flux density. The iron core becomes magnetized, enhancing the magnetic field around the conductor.

  • What is magnetic permeability and how is it related to relative permeability?

    -Magnetic permeability (mu) refers to the ability of a material to concentrate magnetic lines of flux. Relative permeability (Mu_r) is the ratio of the permeability of a material to the permeability of a vacuum (mu_0). It indicates how easily a material can be magnetized compared to a vacuum.

  • What is the significance of the excitation current test in transformer maintenance?

    -The excitation current test is significant for detecting possible winding or core problems in transformers, even when other tests like turn ratio and winding resistance tests appear normal. It can identify issues such as abnormal core grounds, winding faults, and manufacturing defects.

  • Why can't we measure the magnetic flux directly in a transformer?

    -Direct measurement of magnetic flux is not possible because it would require being inside the transformer while it is energized. Instead, magnetizing current, which is easier to measure and record, is used as an indicator.

  • What are the typical phase patterns observed during excitation current testing on three-phase transformers?

    -The typical phase patterns observed are the high-low-high pattern, the low-high-low pattern, and the pattern where all phases provide similar measurements. These patterns are tied to the core configuration and the interaction of the magnetic field with the core.

  • How should the excitation current test be performed on a three-phase transformer with a Y connection?

    -For a three-phase Y connection, the test should be performed by measuring each phase (H1 to Ho, H2 to Ho, H3 to Ho) in the ungrounded specimen test (UST) mode. Safety should be observed for other windings, and terminals that are normally grounded should be grounded during the test.

  • What does an unusual excitation current test result suggest?

    -Unusual results from the excitation current test may suggest potential problems with the transformer, such as residual magnetism, winding faults, or core issues. It may be necessary to demagnetize the transformer and repeat the test for accurate results.

Outlines

00:00

๐ŸŽ“ Introduction to Transformer Excitation Current Testing

The webinar, directed by Tom Sandry, delves into the principles of transformer excitation current testing. It covers the basics of magnetism, magnetic flux, electromagnetism, and the importance of understanding these concepts for the test. The session explains the role of magnetic fields, the concept of magnetic flux denoted by ฮฆ (Phi) measured in Weber, and the impact of materials on magnetic permeability. It also demonstrates how an electromagnet works and touches on the concepts of magnetomotive force (MMF), reluctance, and their relationship with magnetic flux.

05:01

๐Ÿงฒ Magnetic Concepts and Transformer Operation

This segment continues the discussion on magnetism, introducing the concept of magnetic permeability and its relevance to materials' ability to concentrate magnetic flux. It explains the calculation of relative permeability (ฮผ_r) and the impact of an iron core on a coil's magnetic flux. The paragraph also covers the principles of magnetomotive force (MMF), reluctance (R), and their interplay in a magnetic circuit, drawing parallels with electrical concepts like EMF and resistance.

10:02

๐ŸŒ€ Faraday's Law and Lenz's Law in Electromagnetic Induction

The third paragraph focuses on electromagnetic induction, a phenomenon discovered by Michael Faraday. It explains how a voltage is induced in a conductor when it cuts through magnetic lines of force. Faraday's law of induced voltage is introduced, highlighting its dependency on the number of coil turns and the rate of change of magnetic flux. Lenz's law is also discussed, illustrating how the induced voltage opposes the change causing the induction, with a demonstration showing the effect of a magnetic field on a falling magnetized object.

15:04

๐Ÿ”Œ Excitation Current Testing for Transformers

This section discusses the importance of excitation current testing in transformers, which can reveal winding or core issues even when other tests seem normal. It explains the physics behind the test, where applying a voltage to a transformer winding generates a magnetic field that affects the transformer's core. The concept of excitation current is introduced, which is the current needed to establish magnetic flux when the secondary side is open. The paragraph also touches on the effects of loading the transformer and how it influences the excitation current.

20:07

๐Ÿ” Detecting Faults Using Excitation Current Test

The paragraph explains how the excitation current test can be used to identify various types of faults in transformers, such as turn-to-turn faults and grounded windings. It describes how a fault in the secondary winding increases the excitation current due to the opposing flux created by the fault. The effects of an autotransformer and core problems on the excitation current are also discussed, with an emphasis on the patterns that may indicate issues within a three-phase transformer.

25:08

๐Ÿ“ˆ Phase Patterns and Test Procedures for Transformers

This section delves into the analysis of phase patterns in three-phase transformers, which can indicate the health of the transformer's core configuration. It outlines the expected patterns and what deviations from these might suggest in terms of potential problems. The procedures for performing excitation current tests on both single-phase and three-phase transformers are detailed, emphasizing safety and the importance of correct test setup and execution.

30:10

๐Ÿ“Š Analyzing Test Results and Conducting the Webinar Quiz

The final paragraph focuses on the analysis of excitation current test results, providing criteria for evaluating the differences in readings and what they might indicate about the transformer's condition. It also mentions the importance of comparing results with previous tests and performing alternate tests if unusual results are obtained. The webinar concludes with a quiz to reinforce the understanding of key concepts covered during the session.

35:10

๐Ÿ Conclusion and Q&A Session

The webinar concludes with a thank you note to the attendees for their participation throughout the year. The director expresses gratitude and emphasizes the pleasure of conducting these educational sessions. The final part of the webinar is dedicated to a Q&A session where participants can ask questions and seek clarifications on the discussed topics.

Mindmap

Keywords

๐Ÿ’กMagnetism

Magnetism is a fundamental concept in the video, defined as the force of attraction or repulsion that arises between objects due to their magnetic properties. It is related to the video's theme as it underpins the understanding of transformer excitation current testing. In the script, magnetism is described through the concept of magnetic fields and lines of force, which are essential for comprehending how transformers operate and why excitation current tests are conducted.

๐Ÿ’กMagnetic Flux

Magnetic flux, denoted by the symbol 'ฮฆ' in the script, refers to the measure of the magnetic field that passes through a given area. It is a key concept in the video because it is directly related to the operation of transformers and the excitation current testing. The script explains that magnetic flux is the number of magnetic field lines emitted from the North Pole of a magnet, with one Weber being equal to 10^8 power magnetic field lines.

๐Ÿ’กElectromagnetism

Electromagnetism is the physics of electromagnetic phenomena, including the relationship between electricity and magnetism. In the video, it is mentioned that the Danish scientist ร˜rsted discovered in 1819 that an electric current flowing through a conductor produces a magnetic field around it. This principle is crucial for understanding how transformers work and why excitation current tests are necessary for diagnosing transformer issues.

๐Ÿ’กMagnetic Permeability

Magnetic permeability, symbolized as 'ฮผ' in the script, is a measure of how easily a material can concentrate magnetic lines of flux. It is akin to conductivity in electrical terms. The script explains that materials with high permeability can be easily magnetized. This concept is important in the video's context as it influences the design and operation of transformers, affecting how excitation current tests are interpreted.

๐Ÿ’กMagnetomotive Force (MMF)

Magnetomotive force, or MMF, is the driving force that produces a magnetic field in a coil, analogous to voltage in an electrical circuit. The script describes it as being dependent on the current flowing through the turns of a coil. MMF is crucial for the excitation current testing as it helps determine the strength of the magnetic field within a transformer, which is key to diagnosing potential faults.

๐Ÿ’กReluctance

Reluctance, symbolized by 'R' in the script, is the opposition to the production of magnetic flux in a material, similar to resistance in electrical circuits. It is calculated as the ratio of magnetomotive force to magnetic flux. The script explains that reluctance is affected by the material's permeability, the length of the coil, and the cross-sectional area. Understanding reluctance is essential for analyzing the results of excitation current tests.

๐Ÿ’กMagnetic Induction

Magnetic induction, discovered by Michael Faraday in 1831, is the process by which a voltage or EMF is induced in a conductor when it cuts across magnetic lines of force. The script discusses Faraday's law of induced voltage, which is central to the operation of transformers and the excitation current tests. The induced voltage is a key factor in diagnosing transformer conditions through these tests.

๐Ÿ’กLenz's Law

Lenz's Law, as mentioned in the script, determines the polarity of the induced voltage and states that the induced current will flow in such a direction as to oppose the change in magnetic flux that produced it. This law is crucial for understanding how transformers respond to changes in current and voltage, which is directly relevant to the excitation current testing process.

๐Ÿ’กTransformer

A transformer, as described in the script, is a device that allows energy transfer from one electrical circuit to another. The ideal transformer would have zero losses, but in reality, there are elements that dissipate energy, such as copper losses, leakage flux, and iron losses. The script emphasizes that changes in these losses can indicate changes in the transformer's internal state, which is why excitation current tests are performed to detect potential problems.

๐Ÿ’กExcitation Current Test

The excitation current test is a diagnostic procedure used to detect winding or core problems in transformers. The script explains that this test is conducted even when other tests like turn ratio and winding resistance tests appear normal. The test involves applying a voltage to a transformer's winding and measuring the resulting current, which can indicate issues like shorts, open circuits, or manufacturing defects. The video's theme revolves around the importance and methodology of performing this test.

Highlights

Introduction to webinar on Transformer excitation current testing by Tom Sandry, Director of Workforce Development at Vector power.

Importance of understanding magnetism for excitation current testing.

Explanation of magnetic field lines and their relation to magnetic poles.

Magnetic flux defined and its measurement in Weber.

Historical discovery of electromagnetism by Hans Christian ร˜rsted.

Demonstration of electromagnetism through a conductor and the left-hand rule.

Magnetic permeability and its comparison to electrical conductivity.

Magnetomotive force (MMF) and its calculation in ampere-turns.

Reluctance in magnetism and its relationship to resistance in electricity.

Magnetic circuit comparison to an electric circuit with EMF and voltage.

Faraday's law of electromagnetic induction and its formula.

Lenz's Law and its demonstration with a magnetized bobbin in a metallic tube.

Transformer energy transfer and the concept of an ideal transformer.

Purpose of excitation current tests in detecting winding and core problems in transformers.

Explanation of how a loaded transformer affects excitation current.

Identification of turns-to-turn faults in transformers using excitation current tests.

Detection of grounded windings in transformers through excitation current tests.

Effects of auto-transformers on excitation current tests.

Analysis of phase patterns in three-phase transformers for fault detection.

Procedure for performing excitation current tests on single-phase and three-phase transformers.

Analysis of test results and comparison with previous data for fault detection.

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Transcripts

play00:00

well hello and welcome to our webinar

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today I am Tom Sandry I am the director

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of Workforce Development at Vector power

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and today we're going to be taking a

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look at Transformer excitation current

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testing

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so without further too let's get

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started

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the topics that we will be covering

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today will be a refresher on magnetism

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since a great deal of the theory behind

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excitation current testing resides in an

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understanding of

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magnetism we will also talk about

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magnetic

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induction lens's

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law we'll discuss why do we perform

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excitation current tests what type of

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information

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do they provide

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us we'll look at understanding the

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physics behind the

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test we will look at finding faults

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using the excitation current

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test understanding phase patterns that

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are created when performing the

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excitation current

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test and finally performing the test and

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the necessary connections

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now every magnet is surrounded by a

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magnetic field that consists of magnetic

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field lines that extend from one end of

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the magnet to the other as well as

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inside the magnet a magnetic field can

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be thought of as consisting of lines of

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force these magnetic field lines are

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said to exit the North Pole of the

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magnet and enter the South Pole the

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forces of magnetic attraction and

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repulsion move along the lines of

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force next let's discuss magnetic

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flux the group or number of magnetic

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field lines that are emitted outward

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from the North Pole of a magnet is

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called magnetic

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flux the symbol for magnetic flux is

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fi

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the international symbol of units or SI

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unit of magnetic flux is called the

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Weber one Weber is equal to 1 * 10 8

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power magnetic field

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lines now let's look at Electro

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magnetism the relationship between

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magnetism and electrical current was

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discovered by a Danish scientist name

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orad in

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1819 he found that if an electric

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current was caused to flow through a

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conductor the conductor produced a

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magnetic field around that

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conductor a convenient way to determine

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the relationship between the current

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flow through a conductor and the

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direction of the magnetic lines of force

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around the conductor is the leftand rule

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for current carrying conductors as seen

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in this

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illustration if you were to

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theoretically grab the conductor with

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your left hand and your thumb pointing

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to the positive potential your fingers

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around the conductor will indicate the

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direction of the magnetic

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field bending a straight conductor into

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a loop has two results magnetic field

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lines become denser inside inside the

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loop and two all lines inside the loop

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are aiding in the same direction when a

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conductor is shaped into several Loops

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it is considered to be a coil to

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determine the polarity of a coil use the

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leftand rule for coils as seen in this

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illustration adding an iron core inside

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a coil will increase the flux density

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the polarity of the iron core will be

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the same as that of the coil current

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flow is from the negative side of the

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voltage source through the coil and back

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to the positive side of the source as

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seen

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here all right let's see a short

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demonstration of an

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electromagnet

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with no potential applied no current

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flows through the

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coil when we apply potential current now

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flows through the coil creating a

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magnetic

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field

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once again with no potential no current

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flows no magnetic field is

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formed once we apply a voltage current

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will

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flow and magnetism is

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formed so let's talk a little bit about

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magnetic

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permeability in the world of magnetism

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magnetic permeability is very similar in

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concept to conductivity in the

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electrical

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World permeability or mu refers to the

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ability of a material to concentrate

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magnetic lines of flux those materials

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that can be easily magnetize are

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considered to have a high

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permeability relative per permeability

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is the ratio of the permeability of a

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material to the permeability of a vacuum

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or mu

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subo the symbol for relative

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permeability is Mu

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subr where mu subr equals mu / mu sub

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o and here we can see the mathematic

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representation for Mu

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subo

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magnetomotive

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force magnetomotive force or MMF is the

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strength of a magnetic field in a coil

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of wire this is dependent on how much

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current flows in the turns of coil the

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more current the stronger the magnetic

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field the more turns of wire the more

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concentrated the lines of force the

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current times the number of turns of the

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coil is expressed in units called

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ampere turns or simply a t also known as

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MMF the equation shown here is the

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mathematical representation for ampere

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hour

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turns

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reluctance as we may have learned in the

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fundamentals of electricity resistance

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is the opposition to current flow in

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magnetism the opposition to the

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production of flux in a material is

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called

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reluctance which corresponds to

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resistance the symbol for reluctance is

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capital letter r and it has the units of

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ampere turns per

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Weber reluctance is related to

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magnetomotive force MMF and flux F by

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the relationship shown in the equation

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equ seen

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here reluctance is inversely

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proportional to

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permeability iron cores have high

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permeability and therefore low

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reluctance air has low permeability and

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therefore High

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reluctance as we see permeability

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reluctance and flux in the magnetic

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world are very similar similar in

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concept to conductivity resistance and

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current in the electrical

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World a magnetic circuit can be compared

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with an electric current in which EMF or

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voltage produces a current flow the

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Ampere turns or magnetomotive force will

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produce a magnetic flux as we see in

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this

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illustration

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the MMF can be compared with EMF and

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flux can be compared to current the

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equation shown is the mathematical

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representation of magnetomotive force

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derived using ohms law or current equals

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voltage / by

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resistance in the magnetic world the

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magnetic flux will

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equal the magnet in a motive force or

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MMF divided by the

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reluctance reluctance will be affected

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by the length of the coil permeability

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of the magnetic material and the

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cross-sectional area of the

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coil next let's take a refresher on

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magnetic

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induction a electromagnetic induction

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was discovered by Michael Faraday in

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1831 Faraday found that if a conductor

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cuts across lines of magnetic force or

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if magnetic lines of force cut across a

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conductor a voltage or EMF is induced

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into the

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conductor consider a magnet with its

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lines of force from the North Pole to

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the South Pole inserted in and out of a

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coil or conductor that is connected to a

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galvanometer which can detect the

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presence of voltage or an EMF when the

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magnet is not moving zero EMF is

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indicated by the

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galvanometer when the magnetic is either

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inserted or retracted a voltage is

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induced into the

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conductor now let's take a close look at

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Faraday's law of induced

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voltage the magnitude of the induced

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voltage depends on two factors one the

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number of turns of a coil and two how

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fast the conductor cuts across the

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magnetic lines of force or flux the

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equation shown is the mathematical

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representation for Faraday's law of

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induced

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voltage where V sub IND D is the induced

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voltage in

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volts n is the number of turns in a

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coil Delta F / delta T is the rate at

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which the flux cuts across the

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conductor and it is expressed in Webbers

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per

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second next let's look at lens's Law

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lens's law determines the polarity of

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the induced voltage induced voltage has

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a polarity that will oppose the change

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causing the induction when current flows

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due to induced voltage a magnetic field

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is set up around that conductor so that

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the conductor's magnetic field reacts

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with the external magnetic field this

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produces the induced voltage to oppose

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the change in the external magnetic

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field field the negative sign in the

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equation shown is an indication that the

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EMF is in such a direction as to produce

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a current whose flux if added to the

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original flux would reduce the magnitude

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of the

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EMF lens's loss States an

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electromagnetic field interacting with a

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conductor will generate electrical

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current that induces a counter magnetic

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field that opposes the magnetic field

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generating the

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current next let's watch a demonstration

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of lens's

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law we have two bobbits of equal size

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and weight one is not

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magnetized the other is

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magnetized

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taking the non-magnetized

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bobbit we will drop it down the center

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of a metallic

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tube notice how it drops based on a

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speed created by its weight and

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gravity now taking the magnetized we

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will insert it and drop it down the

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metallic tube or conductive

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tube here we can see the magnetic field

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opposing the

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induction and that is lens's

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law all right moving on from magnitud

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ISM let's talk a little bit about the

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Transformer or the ideal

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Transformer Transformers allow energy

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transfer from one electrical circuit to

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another for a perfect Transformer there

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would be zero losses or simply energy in

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would equal the energy

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out now in reality a Transformer has

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lots of elements that dissipate energy

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while the unit is energized these losses

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include copper losses leakage flux

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reluctance and iron

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losses losses are all tied to the design

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and construction of the

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Transformer a change in the loss is

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measured therefore shows us a change in

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the internal state of the

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Transformer

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so let's talk a little bit now about why

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we perform excitation current

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tests well Transformer excitation

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current tests are helpful in determining

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possible winding or core problems in

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Transformers even when turns ratio and

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winding resistance tests appear to be

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normal the test allows us to

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detect abnormal core

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grounds winding faults such as shorts

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and open

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circuits load tap changer

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problems and Manufacturing

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defects excitation tests are commonly

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conducted routinely along with power

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factor testing of the

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Transformer under understanding the

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physics when we apply a voltage to one

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winding of a transformer we cause a

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current to flow through that winding the

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current generates a magnetic field

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around the core of the Transformer the

play17:12

magnetic field generates changes in the

play17:15

magnetic state of the Transformer's core

play17:19

magnetic energy begins to circulate in

play17:21

the core this is the magnetic flux when

play17:25

the secondary side of the Transformer is

play17:29

open only as much current as is needed

play17:32

to get flux moving enters the

play17:35

windings this is called the excitation

play17:40

current so why don't we measure the flux

play17:44

directly well simply we can't you would

play17:48

have to be inside the Transformer while

play17:50

it was

play17:51

energized magnetizing current on the

play17:54

other hand is easy to measure and record

play17:58

now we need to keep in mind that the

play18:01

magnetizing current will be voltage

play18:04

sensitive therefore comparisons will

play18:07

require that the same test voltage be

play18:11

applied every

play18:13

time if a load is connected the

play18:16

secondary will pick up power and

play18:18

transfer it through the load the load

play18:21

shows up a reluctance the magnetic

play18:25

equivalent of

play18:27

resistance all right let's break it down

play18:29

one when a load is placed on the

play18:32

secondary winding a current will

play18:34

flow the secondary current I sub 2 will

play18:38

equal the secondary voltage V sub 2 / by

play18:42

the resistance of the secondary or R sub

play18:46

2 second the current on the secondary

play18:50

will in turn create an opposing magnetic

play18:54

flux and three the generator which

play18:57

regulat Ates voltage at a set level will

play19:01

provide more current to maintain the

play19:03

core magnetized equal to the opposing

play19:06

flux or the excitation current will

play19:10

equal the magnitude of the current plus

play19:15

the secondary current I sub

play19:19

2 therefore a loaded Transformer would

play19:23

require more current to be injected by

play19:26

measuring the current we could tell if

play19:29

the Transformer was intentionally

play19:35

loaded so let's talk about the

play19:39

excitation current test being used to

play19:41

find a turns to turn

play19:44

fault if a fault were to develop in the

play19:47

secondary winding of the Transformer

play19:50

this fault would act as a load across

play19:52

the faulted windings drawing a

play19:55

current I sub faal as a result the

play19:59

excitation current would go up due to

play20:02

the opposing flux created by the

play20:06

fault the result of a turnto turn fault

play20:10

in the secondary winding would be a

play20:12

fault current that causes excitation

play20:15

current to

play20:21

increase how about finding grounded

play20:25

windings the excitation current test is

play20:28

also ideal for finding these grounded

play20:30

windings if there is a fault in the

play20:32

windings you'll get circulating current

play20:35

between those turns and the magnetizing

play20:38

current plus the fault

play20:41

current if the secondary winding has a

play20:45

grounded neutral and one of the windings

play20:48

develops a fault to ground the grounded

play20:51

winding will draw a fault current as a

play20:55

result the excitation current will will

play20:58

go up due to the opposing flux created

play21:02

by the

play21:04

fault a grounded winding on a

play21:07

Transformer with a grounded neutral will

play21:10

cause the excitation current to

play21:19

increase how about the effects of

play21:22

preventative autot

play21:25

Transformer most perhaps all tap

play21:27

changers have an autot transformer for

play21:31

transitioning there are certain steps in

play21:33

the low changer where this Auto

play21:36

Transformers is inserted into the

play21:38

windings with these low tap Changers you

play21:41

will have the magnetizing current plus

play21:44

the current in the autot Transformer

play21:46

resulting in a higher excitation

play21:50

current when an autot Transformer is

play21:52

connected across two Taps it acts as a

play21:55

load and the primary current goes up up

play21:59

as Taps are steep through this can

play22:02

create a recognizable step

play22:06

pattern when a low tap changer

play22:08

transitioning device such as a

play22:10

preventative Auto Transformer is in the

play22:13

bridging position the excitation current

play22:16

goes

play22:21

up now the excitation current test is

play22:24

also ideal for finding core problems

play22:29

they will sometimes show up on the

play22:31

difference in current very few of the

play22:34

tests we do on a Transformer can find a

play22:36

cure problem now the swep frequency

play22:40

response analysis test can do this but

play22:45

you need a previous test result or a

play22:49

sfra signature in order to compare

play22:55

to the excitation current test results

play22:58

present

play23:01

patterns for three-phase Transformers

play23:03

there are two patterns the first is

play23:06

between phases two similar High readings

play23:10

and one low reading with some

play23:14

exceptions the second pattern is within

play23:17

each phase when tap changes are

play23:21

present this second pattern will depend

play23:23

upon the tap changer type and

play23:26

manufacturer

play23:28

within each phase you will have similar

play23:31

readings for each tap when the autot

play23:34

Transformer is in your current may go up

play23:38

so it may be one raised to one lower

play23:41

consistently increasing current you may

play23:44

see current go up and down within the

play23:46

phase depending on which tap you're on

play23:49

but you should see a definite

play23:54

pattern for single face Transformers you

play23:57

you'll need a reverse measurement for

play24:01

confirmation you'll perform a forward

play24:04

and reverse test and those two readings

play24:07

should render very similar

play24:13

results so let's talk a little bit about

play24:16

phase

play24:18

patterns the currents Watts measured on

play24:21

a three-phase unit will show a pattern

play24:25

across the

play24:26

phases there are three expected patterns

play24:30

the high reading low reading High

play24:33

reading

play24:34

pattern the low reading High reading low

play24:39

reading

play24:40

pattern and where All Phases will

play24:44

provide similar

play24:48

measurements the phase pattern is tied

play24:51

to both the measurement and the core

play24:55

configuration patterns arise from the

play24:58

core

play25:01

configuration recall that an increased

play25:03

load leads to an increase reluctance and

play25:07

thus an increased current

play25:12

injected interacting with the core at

play25:14

different points will result in

play25:17

different reluctances and thus different

play25:23

currents reluctance sums similar to

play25:31

resistance so in a magnetic core the

play25:34

reluctance of the steel acts much the

play25:37

same to resist magnetic flux as a

play25:41

resistor does to current a magnetic core

play25:44

can be represented by a reluctance

play25:47

circuit for Simplicity assume that each

play25:51

section has a reluctance of 1

play25:56

ohm

play25:59

so to simplify this

play26:02

circuit we would start with taking the

play26:06

three 1 ohm resistors in series as we

play26:09

see

play26:10

circled this would provide us the

play26:13

equivalent Circuit of the 1 ohm resistor

play26:17

now in parallel with 3 ohms providing us

play26:23

75

play26:25

ohms simplifying the circuit even

play26:27

farther we see now we have 1 ohm in

play26:31

series with 75 ohms in series with 1 ohm

play26:35

resulting in

play26:37

3.75 ohms of

play26:40

reluctance now the same will hold true

play26:43

when you energize the cphase

play26:46

so both outer phases in this scenario

play26:50

would result in

play26:52

3.75 ohms of

play26:56

reluctance

play26:59

now when looking at the center

play27:02

phase we can start with the three series

play27:06

there three 1 ohm resistors in

play27:09

series on the A and on the B side so

play27:13

this would simplify down to 3 ohms in

play27:17

parallel with 1 ohm in parallel with 3

play27:20

ohms which would simplify down to

play27:24

1.5

play27:26

ohms this would provide a reluctance of

play27:30

2.50

play27:32

ohms so here we see the outer legs a

play27:37

high

play27:39

reluctance the center leg a lower

play27:48

reluctance now phase pattern

play27:53

characteristics the high low high

play27:56

pattern outer phases have higher

play27:59

currents than the center phase in this

play28:03

pattern typically this is seen in

play28:06

three-leg core type

play28:11

Transformers the low high low

play28:14

pattern the outer phases have lower

play28:17

currents than the center

play28:19

phase this is typically seen in a

play28:22

three-leg y core type Transformers with

play28:26

inaccessible

play28:28

neutrals or three-leg Delta core type

play28:32

without the third phase

play28:36

grounded All Phases being

play28:39

similar we see this in three singlephase

play28:42

Transformers connected as a three-phase

play28:46

bank

play28:49

Transformer anything else than these

play28:52

patterns points to a potential problem

play28:56

or a capacity positive

play29:03

winding performing the

play29:07

test first remove the short circuit

play29:09

jumpers that were used during the power

play29:12

factor test where all the high side

play29:15

windings were jumpered together and all

play29:18

the low side windings were jumpered

play29:20

together excitation current tests are

play29:23

singlephase

play29:26

tests

play29:28

set up the test connections on the high

play29:30

side observe safety for the other

play29:35

windings proceed according to

play29:37

Transformer winding configuration a

play29:40

delta or

play29:43

y ground any terminals that are normally

play29:46

grounded during the test on the windings

play29:48

that are not being energized for example

play29:51

neutral on a y

play29:54

Transformer ground any terminals that

play29:56

would normally be be grounded normally

play29:59

they would be on the low side for

play30:01

example if the Y is on the low side you

play30:03

would ground that

play30:06

connection perform all the tests on the

play30:09

power factor test set using the us or

play30:13

ungrounded specimen test mode of

play30:19

operation now when tap changes are

play30:22

present test as

play30:25

follows for benchmark or base

play30:29

measurements loow tap changer only test

play30:32

all

play30:34

positions no load tap changer only test

play30:38

all

play30:40

positions load tap changer and no load

play30:43

tap changer test all load tap changer

play30:47

positions with the no load tap changer

play30:50

in Center position then all positions in

play30:54

the no loow tap changer with with the

play30:57

low tap changer in

play31:02

neutral for testing on a routine

play31:07

basis non-load tap changer only test as

play31:11

found or on the position regularly

play31:16

tapped for loow tap changer

play31:19

only test one full range all the raises

play31:23

and lowers plus the neutral position and

play31:26

one position in the opposite

play31:30

range for low tap changer and non-load

play31:33

tap changer again test as found or on

play31:37

the position regularly tapped testing

play31:40

the low tap changer one full range plus

play31:44

neutral and one position in the opposite

play31:53

range perform tests at the highest

play31:56

voltage p

play31:58

possible test the phase demanding the

play32:01

highest current first we normally start

play32:04

with H3 to

play32:07

H1 test each phase at the same

play32:12

voltage perform subsequent tests at the

play32:15

same voltage for

play32:19

comparison if you have previous test

play32:22

data we would like the test voltage to

play32:25

be the same as the pre previous year or

play32:28

test

play32:31

date if a preventative Auto Transformers

play32:34

is included in the Transformer it might

play32:37

not be possible to excite that position

play32:40

of the low tap changer testing might be

play32:43

possible with the preventative autot

play32:45

Transformer Bypass or at a lower

play32:50

voltage if the test set trips choose a

play32:53

lower voltage and repeat all three

play32:56

phases

play32:59

never allow test voltage to exceed rate

play33:02

Line to Line of delta or line to ground

play33:05

for

play33:08

y all right let's take a look at some

play33:11

procedures let's first look at a single

play33:16

phase here we will measure H1 to Ho

play33:21

divided by

play33:23

H2 the mode of operation on the power

play33:25

factor test set is we set to the

play33:29

us we will energize

play33:32

H1 our measurement lead will be placed

play33:35

on

play33:36

ho and we will ground XO and leave X2

play33:41

floating

play33:49

open next we will measure ho / H2 to

play33:55

H1

play33:57

once again the mode will be

play33:59

us we will energize the ho we will

play34:03

measure on the

play34:05

H1 and we will ground XO and we will

play34:09

float

play34:10

X2 so for our single phase here is our

play34:14

reverse measurement we should render

play34:17

comparable results to our previous

play34:24

measurement all right our procedure for

play34:26

a three-phase is

play34:28

y we will measure first H1 to

play34:31

Ho in US mode we will energize

play34:36

H1 measurement lead on ho grounding XO

play34:41

and all other terminals

play34:47

floating next we will measure H2 to

play34:51

H we'll energize on H2 measure on ho

play34:57

grounding EXO and floating all other

play35:06

Terminals and finally we will measure H3

play35:09

to Ho we'll energize on

play35:13

H3 measurement lead on ho grounding the

play35:17

XO and all other terminals

play35:25

floating all right let's look at the

play35:27

procedure for three-phase Delta the a

play35:31

phase so here we will measure H3 to

play35:36

H1 we will energize on H3 our

play35:41

measurement lead will be on

play35:43

H1 and we will ground

play35:47

H2 and also

play35:49

XO all the other terminals we will leave

play35:55

floating

play35:59

now the B phase we'll measure H1 to

play36:04

H2 energizing on H1 low voltage lead on

play36:10

H2 we will ground H3 and XO and all

play36:16

other terminals

play36:21

floating and finally the cphase on the

play36:25

Delta we'll measure H2 to

play36:28

H3 energizing on H2 measurement lead on

play36:33

H3 grounding H1 and XO and all other

play36:39

terminals

play36:47

floating now let's take a look at

play36:50

analysis of the test

play36:52

results check the pattern two similar

play36:56

High readings and one low reading is

play36:59

normal though there are some

play37:03

exceptions when T changes are present

play37:06

consider the pattern within the

play37:10

phase for three-phase units compare High

play37:14

readings with the following

play37:17

criteria readings that are less than or

play37:20

equal to 50

play37:22

milliamps difference should not exceed

play37:25

10%

play37:27

readings greater than 50 milliamps the

play37:31

difference should not exceed

play37:37

5% for singlephase units both readings

play37:41

should be compared using the same

play37:43

criteria as stated

play37:47

previously readings less than or equal

play37:49

to 50 milliamps difference should not

play37:52

exceed

play37:53

10% readings greater than 50 milliamps

play37:56

difference should not exceed

play38:00

5% compare normal test to alternate test

play38:03

results should be similar for a winding

play38:06

in good

play38:09

condition if the core is magnetized an

play38:12

irregular pattern for instance a high

play38:15

medium low reading will be present and

play38:18

you will be unable to compare results

play38:22

effectively a true problem could be

play38:25

masked there for the core should be

play38:28

demagnetized and the test should be

play38:35

repeated compare readings to previous

play38:38

results ensure that the same voltage was

play38:41

used for both tests for consistent

play38:44

numerical

play38:47

comparison if unusual results are

play38:49

obtained consider performing an

play38:52

alternate test to further

play38:55

investigate so here we see an example of

play38:58

an alternate test method being used on a

play39:03

Delta

play39:12

configuration so in review the

play39:14

excitation current test has been

play39:16

effective for detecting and confirming

play39:19

winding and core faults even though in

play39:23

some instances normal turn ratio and

play39:26

winding resistance test results had been

play39:30

obtained a Transformer has lots of

play39:33

elements that dissipate energy while the

play39:35

unit is energized these losses include

play39:39

copper

play39:40

losses leakage

play39:42

flux

play39:44

reluctance iron

play39:47

losses losses are all tied to the design

play39:50

and construction of a transformer a

play39:53

change in the losses measured therefore

play39:55

shows us a change in the internal state

play39:59

of the

play40:03

Transformer Transformer excitation

play40:05

current tests are helpful in determining

play40:07

possible winding or core problems in the

play40:11

Transformer even when ratio and winding

play40:13

resistance tests appear to be normal the

play40:17

test allows us to detect abnormal core

play40:21

grounds winding faults such as shorts

play40:24

and open circuits

play40:26

low tap changer problems and

play40:30

manufacturer

play40:32

defects excitation tests are commonly

play40:35

conducted routinely along with power

play40:38

factor

play40:43

testing so as part of our review let's

play40:48

run a little

play40:49

quiz use

play40:52

the questions function in your uh

play40:56

webinar controls and type in either A B

play41:02

C or

play41:04

D the question is the opposition to the

play41:09

production of flux in a material is

play41:11

called enter a for

play41:14

reluctance B for power factor C for

play41:18

resistance or D

play41:22

insulation enter your answer into the

play41:25

questions function in the webinar

play41:32

controls and the answer is a

play41:41

reluctance question two the excitation

play41:44

current test is also good for

play41:48

finding type in a for low

play41:51

frequency B for

play41:54

contamination C for core problems and D

play41:59

for gas filled

play42:00

voids the excitation current test is

play42:03

also good for

play42:09

finding and the answer is C Core

play42:14

problems it is one of the few tests that

play42:18

will allow us to find core problems in a

play42:23

Transformer question number three

play42:27

which of the following measured patterns

play42:29

indicate a possible

play42:32

problem enter a for the high low high

play42:36

pattern B low high low pattern C for All

play42:42

Phases being similar or D the low medium

play42:46

high

play42:47

pattern which of the following measured

play42:49

patterns indicate a possible

play42:55

problem

play43:02

and the answer should be the low medium

play43:05

high

play43:08

pattern this may indicate residual

play43:12

magnetism and the Transformer should be

play43:16

demagnetized and the test

play43:22

reperform question number four which of

play43:26

the following will the excitation

play43:29

current test not help identify so which

play43:33

of the following will the excitation

play43:34

current test not help in identifying a

play43:39

abnormal core grounds B oil

play43:43

contamination C winding faults such as

play43:47

shorts or open circuits or d low tap

play43:51

changer

play43:53

problems which of the following will the

play43:55

excitation current test not help us

play44:00

identify enter your answer into the

play44:02

questions function in the webinar

play44:10

controls and the answer is oil

play44:14

contamination

play44:21

B question number five excitation

play44:24

current test should be performed using

play44:27

the grounded specimen test or GST test

play44:31

mode on the power factor test set enter

play44:35

a for true or B for

play44:39

false the excitation current test should

play44:42

be performed using the GST test mode on

play44:47

the power factor test

play44:52

set and that is false we always run the

play44:57

excitation current test using the usst

play45:02

ungrounded specimen test mode on the

play45:05

power factor test

play45:12

set

play45:14

and that concludes our webinar today on

play45:18

excitation current

play45:21

testing it's been an absolute pleasure

play45:24

uh this is the last of the webinar for

play45:27

our calendar 2023 year I truly truly

play45:32

thank you all for your attendance

play45:34

participation in these webinars we

play45:37

really do truly enjoy uh doing these

play45:40

webinars for you and we thank you for

play45:43

taking the time out of your busy days to

play45:45

participate with

play45:47

us but without further to do how about

play45:51

we get to the questions and answers

play45:55

section of the webinar

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Transformer TestingExciation CurrentWorkforce DevelopmentMagnetic FieldElectrical TheoryMagnetism RefresherFault DetectionPower FactorVector PowerWebinar