Quantity referred to as 'self-capacitance

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Discussion Overview

The discussion revolves around the concept of 'self-capacitance', particularly in relation to its definition, measurement, and implications in various contexts such as circuit design and theoretical physics. Participants explore the differences between self-capacitance and mutual capacitance, and how self-capacitance can be understood and quantified in practical scenarios.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions the definition of self-capacitance as the charge needed to create a 1 Volt electric field between a surface and a ground plane at infinity, expressing confusion over its theoretical nature.
  • Another participant clarifies that self-capacitance is a theoretical concept where the other plate is considered to be Earth, which is treated as a large conductor at zero potential.
  • A participant introduces a practical approach to modeling self-capacitance in circuits, suggesting that a high resistance can be represented in SPICE with a shunt capacitor to ground, indicating the presence of distributed capacitance.
  • Another participant proposes a method to measure the self-capacitance of a wire by charging it with a DC source and using a charge integrator amplifier to quantify the charge.
  • Discussion includes the behavior of coil inductance and how self-capacitance between windings affects impedance at high frequencies, noting that this can be mitigated by adjusting the winding technique.

Areas of Agreement / Disagreement

Participants express varying levels of understanding and interpretation of self-capacitance, with some agreeing on its theoretical aspects while others seek clarification on practical measurement techniques. No consensus is reached on the best approach to define or measure self-capacitance.

Contextual Notes

Participants acknowledge that self-capacitance is a theoretical construct and that practical measurements may involve assumptions about the surrounding environment and the geometry of conductors. The discussion highlights the complexity of modeling self-capacitance in real-world applications.

bbh2808
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Hi all!

I've got a question about the quantity referred to as 'self-capacitance'. From what I can gather, self-capacitance is the amount of charge necessary to generate a 1 Volt E-field between an arbitrary surface and a ground plane @ infinity. This doesn't make sense to me, but that's why I'm hoping someone here can help me understand it!

Typically when people talk about capacitance, it means 'mutual capacitance', the amount of charge @ the surface of the conductor/volt between two conducting surfaces, which makes a lot more sense to me...

How would one measure the 'self-capacitance' of a conductor of arbitrary geometry?
 
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bbh2808 said:
Hi all!

I've got a question about the quantity referred to as 'self-capacitance'. From what I can gather, self-capacitance is the amount of charge necessary to generate a 1 Volt E-field between an arbitrary surface and a ground plane @ infinity. This doesn't make sense to me, but that's why I'm hoping someone here can help me understand it!

Typically when people talk about capacitance, it means 'mutual capacitance', the amount of charge @ the surface of the conductor/volt between two conducting surfaces, which makes a lot more sense to me...

How would one measure the 'self-capacitance' of a conductor of arbitrary geometry?

Actually you're right! Capacitance can exist only between two conductors. However, the concept of self-capacitance is purely theoretical, in that the other plate is considered to be Earth... as Earth is a very large conductor and hence is considered to be at zero potential w.r.t a charged conductor.

However, in pure theoretical sense the other plate is considered to be located at infinity, but that becomes quite an abstract assumption. Hence, Earth is considered as the other plate or conductor.

Regards,
Shahvir
 


If you use a 1-meg resistance in a real circuit, like in the feedback loop of a high frequency op amp, then the 1 meg resistor should be modeled in SPICE like two 500 k resistors in series, with a shunt 10 pF capacitor to ground in the middle. The shunt capacitance is called the self or distributed capacitance. If you use an air-coil inductance at a very high frequency, it will cross over from being inductive to being capacitive, due to internal turn-to-turn self capacitance.
 


Bob S said:
If you use a 1-meg resistance in a real circuit, like in the feedback loop of a high frequency op amp, then the 1 meg resistor should be modeled in SPICE like two 500 k resistors in series, with a shunt 10 pF capacitor to ground in the middle. The shunt capacitance is called the self or distributed capacitance. If you use an air-coil inductance at a very high frequency, it will cross over from being inductive to being capacitive, due to internal turn-to-turn self capacitance.

This is a good analogy :smile:
 


Ok, but I still have a problem!

How can I measure the self-capacitance of a small length of wire?
 


Suppose you have a foot of wire that has a distributed capacitance of 10 picoFarads to the surroundings. If you touch it with a 1000 volt DC source, you will charge the wire to 10 nanoCoulombs. Then if you touch the wire to a charge integrator amplifier you can measure the charge on the wire.

I attach a sketch of a charge integrator Linear Technology LTC 6084) or equiv. op amp with a 1 picoamp typ leakage current. The 10 nano Coulombs will flow onto the integrating amplifier therough the input resistor and give you 10 volts out (full scale). It will leak off at a 1 pA (1 picoCoulomb per second) rate. Use reset button to zero the capacitor through a 10 meg resistor. Change values of components as necessary.
 

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If you have a coil of wire and you measure the impedance of the coil, it should rise uniformly according to the formula for inductive reactance which is
XL = 2 pi F L

But when you do this there is always a peak in the impedance which then drops steadily as the frequency is increased.
This is due to the capacitance between the windings of the coil. It can be reduced by winding the coil with a space between the winding turns. Doing this raises the self resonant frequency of the coil at the expense of making the coil bigger for a given inductance.

This capacitance is the self capacitance of the coil.
 

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