TIDUFG0 November 2025
The voltage (VS) induced at the output of a Rogowski coil is proportional to the time rate of change of current flowing in the primary conductor (IP). The output voltage has a 90° phase shift and lags input for a sinusoidal input current. Because the output of the Rogowski coil is proportional to the derivative of the instantaneous primary current, an integrator is required to retrieve the original current signal. The output voltage is linear, which can be used without integration in applications requiring only current measurement. For applications requiring measurement of power, the phase difference between current and voltage is important and requires phase shifting of the Rogowski current sensor output. Phase shifting is accomplished using an integrator. A Rogowski integrator can be implemented in two ways:
Rogowski coil output, especially PCB Rogowski coil output, is very low (10μV/A–100μV/A). The low output becomes an issue at lower currents, for example 100mA, where the signal needs to be amplified by (100V/V–500V/V) depending on the coil sensitivity. The active integrator circuitry acts as an attenuator while shifting the current waveforms by 90 degrees. Attenuating the low input signal decreases the accuracy because the signal becomes very low where the signal hits the noise floor of the ADC. The gain of the integrator must be set to unity gain to cancel the integration attenuation at the frequency of interest (50Hz–60Hz). To achieve 90 degrees phase shift and gain of one, passive components must be calculated correctly and the component type must be the right type for math operation. For a discrete approach, thin film resistors and C0G and NP0 capacitors are recommended for high precision applications.