Introduction

Simple Circuit Concepts

Transmission lines

Faraday's law

Near and far fields

Spurious coupling mechanisms

- Direct conduction
- Capacitive coupling -problem
- Capacitive coupling -fixing
- Inductive coupling-problem
- Inductive coupling -fixing by twisted
- Inductive coupling -fixing by coax
- Electromagnetic pickup

- Examples
- Safety & star grounding
- Gnd loop resistance, inductance
- Low frequency behavior
- High frequency behavior
- Troubleshooting
- Methods for removing

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Spurious Coupling via capacitive pickup: the problem

Capacitive pickup, a vulnerability of high impedance circuits, is circumvented by shielding the signal wire. Any two separated conductors form a capacitor. The capacitance is C = 8.8A/d picofarads where A is the area of the conductors and d is their separation. Typical human-scale objects have capacitances of a few picofarads. Consider Fig. 5 where a signal from a sensor travels along conductors to a measuring instrument and there exists another voltage source referenced to the same common. Distributed stray capacitance exists between the signal conductor and the conductor connected to the other voltage source. The other voltage source injects a spurious current I = C d(DV)/dt onto the signal conductor where C is the stray capacitance, DV is the difference in voltages between the two conductors, and d(DV)/dt is the time rate of change of DV. This spurious current (red in Fig. 5) adds to the desired signal current (green in Fig. 5). For example, a 1 pF capacitance connected to a 1 volt pulse that has a 1 microsecond rise-time will inject 1 microampere of unwanted current into the signal circuit when the signal voltage is zero. If the circuit being contaminated is high impedance (i.e., signal current is low-current) this spuriously injected current will be significant and cause interference. On the other hand, if the circuit being contaminated is low impedance (i.e., signal current is high-current), the spuriously injected current will have minimal effect.

Capacitive pickup, a vulnerability of high impedance circuits, is circumvented by shielding the signal wire. Any two separated conductors form a capacitor. The capacitance is C = 8.8A/d picofarads where A is the area of the conductors and d is their separation. Typical human-scale objects have capacitances of a few picofarads. Consider Fig. 5 where a signal from a sensor travels along conductors to a measuring instrument and there exists another voltage source referenced to the same common. Distributed stray capacitance exists between the signal conductor and the conductor connected to the other voltage source. The other voltage source injects a spurious current I = C d(DV)/dt onto the signal conductor where C is the stray capacitance, DV is the difference in voltages between the two conductors, and d(DV)/dt is the time rate of change of DV. This spurious current (red in Fig. 5) adds to the desired signal current (green in Fig. 5). For example, a 1 pF capacitance connected to a 1 volt pulse that has a 1 microsecond rise-time will inject 1 microampere of unwanted current into the signal circuit when the signal voltage is zero. If the circuit being contaminated is high impedance (i.e., signal current is low-current) this spuriously injected current will be significant and cause interference. On the other hand, if the circuit being contaminated is low impedance (i.e., signal current is high-current), the spuriously injected current will have minimal effect.

Fig. 5 Spurious current I =Cd(DV)/dt shown as red from external voltage V couples through stray capacitance C and adds to desired signal current which is shown as green.

Troubleshoot ground loops with ease

and without disconnecting anything!

and without disconnecting anything!

US Patent 7,791,353 B2