Active Guarding
Electrostatic protection techniques isolate high-impedance signal lines from surrounding stray capacitance and environmental interference. In precision capacitive instrumentation, the driven shield consists of an active conductor that surrounds the signal wire and is held at the same voltage potential as the signal itself. By maintaining zero potential difference between the signal and the shield, no current can flow between them.
This eliminates the leakage path that would otherwise degrade the measurement.
Electrical Mechanism
An active buffer amplifier with unity gain replicates the sensor signal voltage onto the surrounding shield layer. The input of the buffer connects to the high-impedance sensor electrode, while the output drives the shield. Because the buffer has high input impedance, it does not load the sensor signal.
Performance Gain
Minimizing parasitic capacitance allows the sensor to operate with higher bandwidth and improved signal-to-noise ratios. Standard coaxial cables introduce high capacitance between the signal core and the grounded shield, which dampens high-frequency signals. When configured as a driven shield, the effective cable capacitance drops to nearly zero, permitting long cable lengths without signal attenuation.
This technique allows remote sensor heads to be installed far from the demodulator electronics.
Operating Limit
Frequency limitations of the buffer amplifier constrain the effectiveness of the shielding at high operation rates. If the buffer introduces a phase shift, a voltage difference arises between the signal and the shield, restoring the stray capacitive loading. This phase lag can cause instability or oscillation in the drive loop if it becomes too large.
High-frequency shield drivers must use amplifiers with wide bandwidths and very low phase delay to avoid these issues. In addition, physical damage to the cable insulation can create a leakage path that defeats the buffer mechanism.