Current Transformer (CT)
Current Transformer (CT)
A current transformer (CT) is
a type of transformer that is used to reduce or multiply
an alternating current (AC). It produces a current in its secondary
which is proportional to the current in its primary.
Current transformers, along with
voltage or potential transformers, are instrument transformers. Instrument
transformers scale the large values of voltage or current to small, standardized values
that are easy to handle for measuring instruments and protective relays.
The instrument transformers isolate measurement or protection circuits from the
high voltage of the primary system. A current transformer provides a secondary
current that is accurately proportional to the current flowing in its primary.
Current transformers are used
extensively for measuring current and monitoring the operation of
the power grid. Along with voltage leads, revenue-grade CTs drive the
electrical utility's watt-hour meter on much larger commercial and
industrial supplies.
High-voltage current transformers are
mounted on porcelain or polymer insulators to isolate them from the ground.
Some CT configurations slip around the bushing of a high-voltage transformer
or circuit breaker, which automatically centers the conductor inside the
CT window.
Current transformers can be mounted
on the low voltage or high voltage leads of a power transformer. Sometimes a
section of a bus bar can be removed to replace a current transformer.
Often, multiple CTs are installed as
a "stack" for various uses. For example, protection devices and
revenue metering may use separate CTs to provide isolation between metering and
protection circuits and allows current transformers with different
characteristics (accuracy, overload performance) to be used for the devices.
The burden (load) impedance should
not exceed the specified maximum value to avoid the secondary voltage exceeding
the limits for the current transformer. The primary current rating of a current
transformer should not be exceeded or the core may enter its non-linear region
and ultimately saturate. This would occur near the end of the first half
of each half (positive and negative) of the AC sine wave in the primary and
would compromise the accuracy
Accuracy.
Accuracy classes for various types of
measurement and at standard loads in the secondary circuit (burdens) are defined
in IEC 61869-1 as classes 0.1, 0.2s, 0.2, 0.5, 0.5s, 1 and 3. The class
designation is an approximate measure of the CT's accuracy. The ratio (primary
to secondary current) error of a Class 1 CT is 1% at rated current; the
ratio error of a Class 0.5 CT is 0.5% or less. Errors in phase are also
important, especially in power measuring circuits. Each class has an allowable
maximum phase error for a specified load impedance.
Current transformers used for
protective relaying also have accuracy requirements at overload currents in
excess of the normal rating to ensure accurate performance of relays during
system faults. A CT with a rating of 2.5L400 specifies with output from its the secondary winding of twenty times its rated secondary current (usually 5 A × 20 = 100 A) and 400 V (IZ drop) its output
accuracy will be within 2.5 percent.
Burden.
The secondary load of a current transformer is termed the "burden" to distinguish it from the primary
load.
The burden in a CT a metering electrical network is a largely resistive impedance presented to its secondary winding.
Typical burden ratings for IEC CTs are 1.5 VA, 3 VA, 5 VA,
10 VA, 15 VA, 20 VA, 30 VA, 45 VA, and 60 VA.
ANSI/IEEE burden ratings are B-0.1, B-0.2, B-0.5, B-1.0, B-2.0 and B-4.0. This
means a CT with a burden rating of B-0.2 will maintain its stated accuracy with
up to 0.2 Ω on the secondary circuit. These
specification diagrams show accuracy parallelograms on a grid incorporating
magnitude and phase angle error scales at the CT's rated burden. Items that
contribute to the burden of a current measurement circuit are switch-blocks,
meters and intermediate conductors. The most common cause of excess burden
impedance is the conductor between the meter and the CT. When
substation meters are located far from the meter cabinets, the excessive length
of cable creates a large resistance. This problem can be reduced by using
thicker cables and CTs with lower secondary currents (1 A), both of which
will produce less voltage drop between the CT and its metering devices.
Knee-point
core-saturation voltage.
The knee-point a voltage of a current transformer is the magnitude of the secondary
voltage above which the output current ceases to linearly follow the input
current within declared accuracy. In testing, if a voltage is applied across
the secondary terminals the magnetizing
current will increase
in proportion to the applied voltage until the knee point is reached. The knee
point is defined as the voltage at which a 10% increase in applied voltage
increases the magnetizing current by 50%. For voltages greater than the
knee point, the magnetizing current increases considerably even for small increments
in voltage across the secondary terminals. The knee-point voltage is less
applicable for metering current transformers as their accuracy is generally
much higher but constrained within a very small range of the current
transformer rating, typically 1.2 to 1.5 times rated current. However, the
concept of knee point voltage is very pertinent to protection current
transformers, since they are necessarily exposed to fault currents of 20 to 30
times rated current.
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