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My question is about the Kelvin equation which is as follows:

$$\ln(e/e_s) = \frac{2\cdot\sigma}{n\cdot k\cdot T\cdot r} $$

Keep in mind that the $e$ in $\ln(e/e_s)$ is not the constant $\mathrm{e}$.

I know that:

$$\frac{e}{e_s} = \mathrm{e}^{(\frac{2\cdot\sigma}{n\cdot k \cdot T \cdot r})}$$

I need to show that this is equal to:

$$\frac{e}{e_s} = 1 + \frac{a}{r}$$

Where $a = \frac{2\cdot \sigma}{n\cdot k\cdot T}$

How do I go about doing this?

1 Answers1

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You want to show that $e^{a/r} = 1 + a/r$. But that isn't true. What is true is that $$ e^{a/r} = 1 + a/r + \frac{a^2}{2!r^2} + \frac{a^3}{3!r^3} + \cdots$$ So if $a/r$ were small, so that $a^2/r^2$ and all the following terms on the right were very small, then $1+a/r$ would be a good approximation for $e^{a/r}$.