| 21. | The spacing between probes must be larger than the Debye length of the plasma to prevent an overlapping Debye sheath.
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| 22. | The associated length ? D a " 1 / " k " 0 is called the Debye length.
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| 23. | When doping profiles exceed the Debye length, majority carriers no longer behave according to the distribution of the dopants.
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| 24. | This model is valid for most aqueous systems because the Debye length is typically only a few nanometers in water.
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| 25. | As can be seen from the above equation, the repulsion energy depends on the square of the Debye length.
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| 26. | At these parameters, the ion Larmor radius is a few millimeters, and the Debye length is tens of micrometres.
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| 27. | This overestimation is visible at distances less than half the Debye length, where the decay is steeper than exponential decay.
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| 28. | The associated increase in the Debye length must be taken into account when considering ion non-saturation due to sheath effects.
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| 29. | The thin DL model is valid for most aqueous systems because the Debye length is only a few nanometers in such cases.
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| 30. | In a nanochannel, however, the solution is charged when the dimension of channel radius is smaller than the Debye length.
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