2010
DOI: 10.1063/1.3357438
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Response to “Comment on ‘Carbon nanowalls as material for electrochemical tranducers’ ” [Appl. Phys. Lett. 96 126102 (2010)]

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Cited by 2 publications
(1 citation statement)
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“…2) of the films grown for various time durations, the distance between the flakes varies from approximately 50-100 (for 30 s growth time) to 500-1,000 nm (for 600 s growth time). Now in order for the Randles-Sevcik equation to be valid, the size of the diffusion layer formed (at a particular scan rate) in the average of each ensemble of nanoflakes should be much higher than the average spacing between them [33,34]. To calculate this, we need to consider the size of the diffusion layer δ surrounding the nanoflake ensemble using the equation δ = (2D×(ΔE/ν) 1/2 ), where D is diffusion constant for the ferrocouple redox probe (7.63×10 −6 cm 2 s −1 , 1 M KCl), ΔE is the potential width of the voltammograms, and ν is the scan rate.…”
Section: Electrochemical Properties Of Flgsmentioning
confidence: 99%
“…2) of the films grown for various time durations, the distance between the flakes varies from approximately 50-100 (for 30 s growth time) to 500-1,000 nm (for 600 s growth time). Now in order for the Randles-Sevcik equation to be valid, the size of the diffusion layer formed (at a particular scan rate) in the average of each ensemble of nanoflakes should be much higher than the average spacing between them [33,34]. To calculate this, we need to consider the size of the diffusion layer δ surrounding the nanoflake ensemble using the equation δ = (2D×(ΔE/ν) 1/2 ), where D is diffusion constant for the ferrocouple redox probe (7.63×10 −6 cm 2 s −1 , 1 M KCl), ΔE is the potential width of the voltammograms, and ν is the scan rate.…”
Section: Electrochemical Properties Of Flgsmentioning
confidence: 99%