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AN3306 bảng dữ liệu(PDF) 12 Page - STMicroelectronics

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Giải thích chi tiết về linh kiện  Current sensing in metering applications using
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AN3306 bảng dữ liệu(HTML) 12 Page - STMicroelectronics

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Benefits of using STPMxx with Rogowski coil-based sensors
AN3306
12/21
Doc ID 18182 Rev 1
Equation 6
The final result is:
Equation 7
This makes the use of STPMxx devices with Rogowski coil-based current sensors, such as
the Pulse current sensor, advantageous. When a Rogowski coil-based sensor is used, a
very high degree of accuracy is obtained by design due to the following:
●
DC offset cancellation and the power calculation algorithm produces a DC component,
proportional to the active power, without any offset or AC ripple.
●
Ripple-free power calculation, so integration of power over the line period is avoided,
and thus energy accumulation is not affected by fluctuation of the line frequency.
●
The architecture makes the STPMxx devices ready for Rogowski coil-based sensors
without the need for an additional integration block, which would increase system
complexity and overall application cost.
5.2
Mutual current compensation
For poly-phase systems, where galvanic isolation between phases is a must, and immunity
to DC magnetic fields is becoming a requirement in international standards, a Rogowski
coil-based sensor offers an interesting and inexpensive solution.
The drawback of this approach is cross influence between current channels.
The STPMC1, a dedicated device for poly-phase measurement, features embedded
functionality which allows error compensation from mutual currents.
For single-phase systems, two correction factors,
α (alpha) and β (beta), produce a ±3.1%
correction factor in 512 steps. Asymmetrical compensation is implemented by multiplying
the phase current with
α and neutral current with β, and these values are then subtracted
from neutral and phase currents, respectively, as shown in Table 3 and Equation 8 and
Equation 9.
Equation 8
Table 3.
Mutual current compensation matrix for single-phase systems
Phase
S
T
S
−β
T
α−



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