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Beyond the Knee Point: a Practical Guide to CT Saturation

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Beyond the Knee Point: a Practical Guide to CT Saturation 1 Beyond the Knee Point: A Practical Guide to CT Saturation Ariana Hargrave, Michael J. Thompson, and Brad Heilman, Schweitzer Engineering Laboratories, Inc. 2350 NE Hopkins Court, Pullman, WA 99163 USA, +1.509.332.1890 Abstract—Current transformer (CT) saturation, while a fairly understanding of CT saturation must extend beyond the common occurrence in protection systems, is not often clearly knee point. understood by protective relay engineers. This paper forgoes the usual physics equations to describe how CTs saturate in a simple and intuitive way. We explain the differences between II. CT SATURATION THEORY symmetrical and asymmetrical saturation and how remanence To understand CT saturation, it is very important to accumulates in the core of a CT. We then describe the CT understand the basic concept of how CTs work and what is equivalent circuit and how it results in the familiar CT excitation actually happening when they saturate. This section describes graph. ANSI ratings of CTs are explained, and we show how to analyze the performance of CTs using simple equations and tools. what happens in the core of a CT during symmetrical saturation, Finally, we explain how CT saturation can affect relay operation asymmetrical saturation, and remanence. It then explains how and show how to detect CT saturation in protective relay event this core activity corresponds to the CT equivalent circuit, reports. Real-world event reports are presented where correct ANSI voltage ratings, and the familiar CT excitation graph. relay operation was compromised as a result of incorrect current values from saturated CTs. A. How CTs Work In its simplest form, a CT consists of two sets of wire I. INTRODUCTION windings around an iron core, as shown in Fig. 1. The concept Current transformer (CT) saturation is not a new topic, and is the same for a window or bushing CT, which consists of a there have been many papers, books, application guides, and secondary winding around a core, with the primary winding tutorials written on the subject. Sorting through this vast array being the primary conductor that passes through it. of information to piece together a complete understanding of Transformers work based on the principle of electromagnetic the topic is a time-consuming task and may not be realistic with induction. This principle states that an alternating magnetic flux the schedules and demands placed on many practicing in the presence of a loop of wire induces a voltage across that engineers. Because of this, engineers’ level of understanding is loop. Magnetic flux is simply the amount of magnetic field often limited to the familiar CT excitation graph. The following passing through a material such as a transformer core. is a list of common questions related to CT saturation: When alternating current IP flows in the primary winding of • Why does a CT saturate (Section II, Subsection B)? a transformer, it generates an alternating magnetic field H, • What is remanence, and do I have to worry about it which corresponds to an alternating magnetic flux Φ, around (Section II, Subsection C)? the transformer core. This alternating magnetic flux passes • What does it mean when a CT is a C800 (Section II, through the secondary winding. What happens next depends on Subsection F)? the load connected to the secondary winding. • I have a C800 multiratio CT tapped at 400/5. Is it still If the secondary is connected to a burden, the alternating a C800 (Section II, Subsection F)? magnetic flux in the core induces an alternating voltage VS across the secondary winding. This causes a corresponding • How do I make sure my CT will not saturate for my alternating current IS to flow in the secondary winding. The worst-case fault current (Section III)? alternating current in the secondary creates its own alternating • The knee point determines the saturation voltage of a magnetic field and alternating magnetic flux that oppose those CT, right (Section II, Subsection E)? created by the primary winding. These primary and secondary • Will saturated CTs cause my relay to misoperate? fluxes cancel, leaving a negligible amount of net flux in the What if they just saturate a little bit (Section V)? core. This occurs until the core becomes saturated. • After a misoperation, how do I know if CT saturation If the secondary is open-circuited, the alternating magnetic was a cause (Section IV)? flux in the core induces a very high alternating voltage VS • Can modern relays prevent misoperations due to CT across the secondary winding. VS remains on the terminals with saturation (Section VI)? no secondary current flowing, which is why it is very dangerous The goal of this paper is to explain CT saturation to the to open-circuit an in-service CT. Because IS cannot flow, it protective relay engineer and to answer these questions in a cannot create an opposing magnetic field, leaving a net flux in clear and practical way. As this paper demonstrates, a proper the core equal to the flux created by the primary current. 2 This magnetic behavior is modeled when we introduce the CT equivalent circuit in Section II, Subsection D. For now, 1 know that the induction of voltage VS is a result of the magnetic field created by IP along with the internal impedances of the transformer and the connected load. For simplification going 0 forward, we assume a fixed linear burden is connected to the CT. When this is the case, Ohm’s law mandates that the secondary current in the CT and the voltage across the –1 magnetizing impedance are directly proportional. Magnetic Flux Density (B) H Φ –10 –5 0 5 10 Magnetic Field Strength (H) IS IP Fig. 2. Example B-H curve How this magnetic behavior affects the ability of the CT to VS reproduce current is simple: it is the change in flux caused by the magnets changing direction that induces voltage VS across the secondary winding of the CT. Voltage VS, in turn, generates current IS through the connected circuit. When the core reaches maximum flux density, it is fully saturated and there are no more magnets remaining to change direction. This causes voltage VS to drop to zero, and current IS ceases to flow. Fig. 1. CT drawing CT saturation can occur in two forms: symmetrical B. Why Does a CT Saturate? saturation and asymmetrical saturation. These saturation types are explained in the following subsections. For a detailed In an ideal world, the secondary current leaving the CT (IS) explanation of the mathematics of CT saturation, see [1]. is an exact replica of the primary current (IP) divided by the ratio of the number of turns in each winding (CT ratio). 1) Symmetrical Saturation However, when a CT saturates, IS does not accurately replicate Symmetrical saturation is the result of a symmetrical IP. The reason a CT saturates is related to what physically primary current being applied to the CT that is too large for the occurs inside a CT during the electromagnetic induction CT core to handle for a given burden. process. The iron core of a CT is made up of a fixed number of Fig. 3 shows an example of the primary current (IP) and magnetic dipoles, which can be thought of as molecular secondary current (IS) of a CT during symmetrical saturation. magnets. Ideally, these magnets are randomly arranged in Ideally, before the current is applied at Point a, the magnets in polarity throughout the core, as shown in Fig. 1. the core are aligned in random directions (no remanence, which When alternating current (IP) flows in the primary winding is discussed later in this paper). Between Points a and b, as IP and generates the magnetic field (H), the strength of this starts to flow in the first positive half cycle, the magnets start to magnetic field affects the magnets in the core and causes them line up in the positive direction. Because there is a change in to start lining up (in the same direction as the magnetic field) to flux during this time, the current IS matches IP exactly produce the magnetic flux (Φ). The more current IP that flows, (assuming a CT ratio of 1:1). Before the positive half cycle is the stronger the magnetic field (H) becomes, and the more over, at Point b, all of the magnets available in the core are lined magnets become lined up. The number of magnets that are lined up in the positive direction, and the core has reached maximum up at a given time is the flux density (B). When all the magnets flux density (saturation). At this point, even though IP continues in the core are aligned in the same direction, the maximum flux to flow, there is no more change in flux, VS drops to zero, and density of the core is reached and the CT core is said to be IS drops to zero. IS stays at zero until IP begins to flow in the saturated. negative direction, reversing the magnetic field. This negative The relationship between the magnetic field strength (H) and flow, beginning at Point c, causes the magnets to begin aligning the magnetic flux density (B) is given by the B-H curve of the in the negative direction. This changing flux allows the core, as shown in the example in Fig. 2. Different types of core generation of voltage VS and allows IS to follow IP again until materials have different B-H curves, which depend on the all of the magnets are aligned in the negative direction at ability of the material to support a magnetic field. Point d.
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