Current transformers (CTs) are indispensable components in electrical power systems, serving as critical interfaces between high-current primary circuits and low-current measuring, metering, and protection devices. Their performance is primarily evaluated by two key parameters: ratio error (inaccuracy in the magnitude of the transformed current) and phase error (discrepancy in the phase relationship between primary and secondary currents). These errors, if unmanaged, can compromise the reliability of power system monitoring, billing accuracy, and the responsiveness of protective relays. This article delves into the underlying mechanisms of ratio error and phase error in CTs, exploring the electrical, magnetic, and structural factors that contribute to their occurrence.
To understand error mechanisms, it is first necessary to distinguish between an ideal CT and a real CT.
Ideal CT: A theoretical model with no energy losses. Its primary current (I1) and secondary current (I2) strictly follow the inverse turns ratio: I1/I2=N2/N1, where N1 is the number of primary turns and N2 is the number of secondary turns. Additionally, the secondary current is perfectly in phase with the primary current (no phase shift).
Real CT: Deviates from the ideal model due to inherent magnetic and electrical losses. These losses introduce both ratio error and phase error, which must be quantified and minimized for accurate operation.
Ratio error (also called transformation error) is the difference between the actual current ratio of a CT and its nominal (rated) ratio. Mathematically, it is expressed as:
Ratio Error (%)=(I1Kn⋅I2−I1)×100
Where:
Kn is the nominal turns ratio (Kn=N2/N1),
I2 is the actual secondary current,
I1 is the primary current.
A positive ratio error indicates that the secondary current is larger than the ideal value, while a negative error means the secondary current is smaller.
Ratio error arises from the imperfect magnetic coupling between the primary and secondary windings, primarily due to magnetizing current and core losses. These factors disrupt the ideal current balance dictated by the turns ratio. Below is a detailed breakdown of the key mechanisms:
The magnetic core of a CT requires a certain amount of current to establish and maintain the alternating magnetic flux (Φ) in the core—this is the magnetizing current (Im). In an ideal CT, the primary current is entirely balanced by the secondary current (i.e., N1I1=N2I2). However, in a real CT, the primary current must supply both the magnetizing current and the current required to balance the secondary current.
Impact on Ratio: The magnetizing current (Im) is a "loss" current that does not contribute to the secondary current. Thus, the primary current can be decomposed as:N1I1=N2I2+N1Im
Rearranging gives:I2=N2N1(I1−Im)
This shows that I2 is smaller than the ideal value (N1I1/N2) by the term (N1/N2)Im, directly introducing a negative ratio error.
Factors Influencing Im:
Core Material: High-permeability materials (e.g., grain-oriented silicon steel) reduce Im by requiring less current to magnetize the core.
Core Geometry: A larger core cross-sectional area lowers flux density (B=Φ/A), reducing Im (since Im is proportional to flux density in the linear region).
Primary Current Level: At low primary currents, the core operates in the non-linear part of the magnetization curve, increasing Im and worsening ratio error.
The alternating magnetic flux in the core induces two types of power losses: hysteresis loss and eddy current loss. These losses are supplied by the primary current, further diverting it from the ideal balance with the secondary current.
Hysteresis Loss: Occurs due to the energy required to reverse the magnetic domains in the core material as the flux alternates. It is proportional to the area of the hysteresis loop and the frequency of the alternating current.
Eddy Current Loss: Caused by induced currents circulating within the core material (due to Faraday’s Law), which dissipate energy as heat. Eddy current loss is minimized by using laminated cores (insulated layers) to reduce current paths.
Combined, hysteresis and eddy current losses create a core loss current (Ic=Ih+Ie), which adds to the magnetizing current (Im) to form the exciting current (I0=Im+Ic). The exciting current is the primary current component responsible for maintaining flux in the core, and it is the root cause of ratio error:
Ratio Error∝I1I0
At low primary currents (e.g., 10–20% of rated current), I0 constitutes a larger fraction of I1, leading to significant ratio error. At high currents (near rated value), I0 is negligible compared to I1, reducing the error.
The secondary burden (Zb) refers to the total impedance of the secondary circuit, including the resistance of the secondary winding (R2), the resistance of connecting wires (Rw), and the impedance of connected devices (e.g., relays, meters, Zload):
Zb=R2+Rw+Zload
Impact on Ratio Error: A higher burden increases the voltage drop across the secondary winding (V2=I2Zb). To maintain this voltage, the core flux must increase (per Faraday’s Law: V2≈4.44fN2Φmax), which requires a larger exciting current (I0). As I0 rises, the ratio error worsens.
CTs are rated for a specific burden (e.g., 5 VA, 10 VA), and exceeding this rating leads to excessive flux and increased error.
Core saturation occurs when the magnetic flux density (B) in the core reaches a point where the material can no longer be magnetized further (the "knee" of the magnetization curve).
Causes: Saturation is triggered by excessive primary current (e.g., during faults) or an overloaded secondary burden (which increases flux demand).
Effect on Ratio Error: In saturation, the core’s permeability drops sharply, causing the exciting current (I0) to increase exponentially. This breaks the linear relationship between I1 and I2, leading to severe ratio error. For example, a CT with a 1000:5 ratio might output only 3A instead of 5A when saturated, resulting in a large negative error.
Real windings have non-zero resistance (R1 for primary, R2 for secondary) and leakage reactance (X1 for primary, X2 for secondary). Leakage reactance arises from magnetic flux that links one winding but not the other, failing to contribute to mutual induction.
Impact: These impedances cause voltage drops in the windings, which must be compensated for by increased flux in the core. This, in turn, increases the exciting current (I0) and introduces small but measurable ratio errors, especially at high frequencies or high currents.
Phase error (or angular error) is the difference in phase angle between the primary current (I1) and the secondary current (I2) (when I2 is reversed to account for the CT’s polarity). In an ideal CT, the reversed secondary current (−I2) is perfectly in phase with I1. In reality, a phase shift (δ) occurs, defined as:
δ=Phase angle of I1−Phase angle of (−I2)
Phase error is typically measured in minutes (1 minute = 1/60 degree) and is considered positive if −I2 lags I1.
Phase error stems from the phase differences between the exciting current components (Im and Ic) and their interaction with the secondary burden.
The exciting current (I0) has two components:
Magnetizing current (Im): Lags the core flux (Φ) by 90° because it is purely reactive (energy stored in the magnetic field is returned to the circuit each cycle).
Core loss current (Ic): Is in phase with the induced voltage (V2) because it represents real power loss (dissipated as heat), making it resistive.
The total exciting current (I0) is the vector sum of Im and Ic, resulting in a phase angle (α) where:
tanα=IcIm
This phase angle of I0 relative to V2 is a primary source of phase error in the CT.
The secondary burden (Zb) is typically a combination of resistance (Rb) and reactance (Xb), with a phase angle (θ) where:
tanθ=RbXb
Inductive Burden: If the burden is inductive (Xb>0), the secondary current (I2) lags V2 by θ. This lag, combined with the phase angle of I0, increases the overall phase error between I1 and −I2.
Resistive Burden: A purely resistive burden (Xb=0) minimizes phase shift, reducing phase error.
The interaction between the exciting current’s phase (α) and the burden’s phase (θ) creates the total phase error (δ), approximated as:
δ≈(π180)(I2N2/N1Imcosθ−Icsinθ) minutes
This formula shows that phase error depends on both the core’s magnetic properties (Im,Ic) and the burden’s impedance characteristics (θ).
In saturated conditions, the magnetizing current (Im) increases drastically and becomes highly non-sinusoidal, with a phase angle that deviates from the ideal 90° lag. This distortion disrupts the linear phase relationship between I1 and I2, causing significant phase error. For protection CTs, which must operate during fault currents (where saturation is common), minimizing phase error under saturation is critical to ensure relays trip at the correct time.
CT performance is rated for a specific frequency (e.g., 50Hz or 60Hz). Deviations from this frequency affect both core losses and reactances:
Hysteresis loss increases with frequency, altering Ic and its phase.
Eddy current loss increases with the square of frequency, further changing Ic.
Leakage reactance (X1,X2) is proportional to frequency, modifying the voltage drops in the windings.
These changes shift the phase relationship between I1 and I2, introducing phase error.
Ratio error and phase error are not independent; they share common root causes in the exciting current and secondary burden. For example:
An increase in secondary burden raises both I0 (worsening ratio error) and shifts the phase of I2 (worsening phase error).
Core saturation amplifies both errors simultaneously, as the exponential rise in I0 disrupts both magnitude and phase relationships.
This interdependence means that design improvements (e.g., using better core materials) often reduce both errors, while operating conditions (e.g., overloading) degrade both.
To reduce ratio and phase errors, CTs are designed and operated with the following considerations:
High-Performance Core Materials: Grain-oriented silicon steel or amorphous alloys minimize Im and core losses (Ic) due to their high permeability and low hysteresis.
Optimal Core Design: Larger cross-sectional areas reduce flux density, lowering Im and saturation risk. Laminated cores (with thin insulation) minimize eddy current losses.
Burden Management: Ensuring the secondary burden stays within the CT’s rated limits (e.g., 5–30 VA) prevents excessive flux and I0 increases.
Winding Optimization: Thick conductors reduce winding resistance (R1,R2), while tight winding configurations minimize leakage reactance (X1,X2).
Accuracy Classes: CTs are rated for specific accuracy classes (e.g., Class 0.1 for precision metering, Class 5P for protection). These classes define maximum allowable ratio and phase errors under rated conditions. For example, a Class 0.5 CT has a maximum ratio error of ±0.5% and phase error of ±20 minutes at rated current.
Ratio error and phase error in current transformers are inherent to their operation, arising from magnetic core characteristics, exciting current components, secondary burden, and winding imperfections. Ratio error is primarily driven by the exciting current (I0), which diverts primary current from the ideal turns ratio balance, while phase error stems from the phase differences between I0 components and the secondary burden’s impedance.
Understanding these mechanisms is critical for selecting appropriate CTs for specific applications (e.g., metering vs. protection), ensuring accurate current measurement, reliable relay operation, and efficient power system management. By optimizing core materials, controlling secondary burden, and adhering to accuracy class standards, engineers can mitigate these errors and enhance the performance of current transformers in electrical systems.