Figure 4-1C shows the profiles that

Figure 4-1C shows the profiles that result when the applied potential is sufficiently negative that the concentration of O at the electrode surface is effectively zero, i e., Co/CK 0.001. In this case, essentially all of O at the electrode surface must be electrolyzed to R in order to satisfy the Nersnt equation. Consequently, O is converted to R as rapidly as it can diffuse to the electrode surface. Since this is a limiting condition, application of even more negative potentials causes only negligible change in the profiles. Although thee transition between stagnant and flowing solution is considered to be abrupt in this example, the transition is in reality gradual. Consequently, the profiles are rounded as shown by the dotted line in Fig.4-1C. However, the hypothetical situation of an abrupt transition is a useful approximation in mathematical treatments.

結果 (繁體中文) 1:

圖 4-1 C 所示的設定檔時所施加的電位是足夠的負 O 在電極表面的濃度是有效零，i，導致 e.，Co/CK 0.001。在這種情況下，基本上所有的 O 在電極表面必須被電解到 R 為了滿足 Nersnt 方程。因此，O 是它可以擴散到電極表面一樣迅速轉換為 R。由於這是一個限制條件，甚至更負電位的應用導致只有微不足道的變化在設定檔中。雖然你之間的過渡停滯和流動的解決方案被認為是突然在此示例中，處於現實逐漸過渡。因此，在圖 4-1 C 虛線所示的舍入設定檔。然而，假設的情況的一個突然是轉變的一個有用的近似數學處理。

結果 (繁體中文) 2:

圖4-1C示出了導致當所施加的電位是足夠負，在電極表面的O的濃度是有效的零的型材，I E。，鈷/ CK 0.001。在這種情況下，基本上所有在電極表面的O必須以滿足Nersnt方程被電解至R。因此，O被轉換至R為快速，因為它可以擴散到電極表面上。由於這是一個限制條件，甚至更負的電位的施加導致在配置文件僅可忽略的變化。雖然停滯和流動溶液之間你過渡被認為是在本實施例中突然，過渡是在現實中漸進的。因此，輪廓是圓形的，如圖由Fig.4-1C虛線。然而，突然轉變的假設情況是在數學治療有用的估計。