Inserting a dielectric material between two plates of a capacitor

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SUMMARY

The discussion centers on the insertion of a dielectric material between the plates of a capacitor and its effects on energy and capacity. The new capacitance is defined by the formula ##C = K \cdot C_{0}##, where K is the dielectric constant. The total work done during this process is calculated as ##W_{tot} = \Delta U = U_{f} - U_{i} = \frac{1}{2} \cdot (K-1)C_{0}V_{0}^2 > 0##, indicating that the capacitor gains potential energy. The energy required for this process is sourced from the power supply, which facilitates the dielectric's insertion, ultimately stabilizing the electric field between the plates.

PREREQUISITES
  • Understanding of capacitor fundamentals, including capacitance and potential energy.
  • Familiarity with dielectric materials and their properties.
  • Knowledge of energy conservation principles in electrical systems.
  • Proficiency in mathematical expressions related to electrical energy calculations.
NEXT STEPS
  • Study the impact of different dielectric materials on capacitor performance.
  • Learn about the relationship between electric field strength and dielectric constant.
  • Explore energy density calculations in capacitors with dielectrics.
  • Investigate the effects of dielectric insertion on capacitor discharge behavior.
USEFUL FOR

Electrical engineers, physics students, and anyone involved in capacitor design or analysis will benefit from this discussion, particularly those interested in the effects of dielectrics on energy storage and stability in capacitors.

idor
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Homework Statement
Is the external mechanical work done by inserting a dielectric material between two plates of a capacitor (plates capacitor) when the power source remains connected always negative?
and if so, does it mean that the process can proceed spontaneously after being initiated?
Relevant Equations
The original capacity is C0, the voltage is V0, and the dielectric constant of the material is K >1.
1566120347488.png

1. new capacity: ##C = K\cdot C_{0}##.
2. initial potential energy: ##U_{i} = \frac 1 2 \cdot C_{0}V_{0}^2##.
3. final potential energy: ##U_{f} = \frac 1 2 \cdot KC_{0}V_{0}^2##.
4. total work done: ##W_{tot} =\Delta U = U_{f} - U_{i} = \frac 1 2 \cdot (K-1)C_{0}V_{0}^2 > 0##.
5. also total work done: ##W_{tot} = W_{p}~\text{(power source work for streaming more charge)} + W_{ext}~\text{(external work for inserting the material).}##
6. power source work: ##W_{p} = \Delta q \cdot V_{0} = (q_{f} - q_{i})V_{0} = (C \cdot V_{0} - C_{0} \cdot V_{0}) \cdot V_{0} = (K-1) \cdot C_{0}V_{0}^2.##
7. external mechanical work: ##W_{ext} = W_{tot} - W_{p} = \frac 1 2 \cdot (K-1) \cdot C_{0}V_{0}^2 - (K-1) \cdot C_{0}V_{0}^2 =
\\= -\frac 1 2 \cdot (K-1)C_{0}V_{0}^2 < 0.##
 
Last edited:
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Hello Idor, ##\qquad## :welcome: ##\qquad## !

Well, you work out your own question immacculately ! For K > 1 you get a definite W < 0.
So: yes !
And it indeed means the capacitor 'pulls in' the dielectric. If the force is enough to overcome friction it will actually do it seemingly spontaneously.

So where does the energy come from ?
 
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Hi,
Thank you very much! your confirmation really helps.

It just seemed odd to me at first that the capacitor would 'pull in' the dielectric material even when the power source remains connected, after looking at a similar example where it was disconnected first, and the total amount of work done was negative because the capacitor lost potential energy.

However, in the second case (my question) the total amount of work done (positive from the power source + negative from the insertion of the material) is positive (as the capacitor gains potential energy), and that is why I wonder what makes this process favorable.

I assume that the energy comes from the power source, but what does the system earn from this?
Is it because the dielectric material lowers the electric field between the plates of the capacitor, and therefore somehow makes the system more stable?
 
Energy density (volumtric) is 1/2 DE. D = ##\epsilon E ##. So the final energy in the capacitor's E field is incremented by ## \epsilon_r = \epsilon/\epsilon_0. ##
 
Last edited:

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