The absorption coefficient \( \alpha \) is given by the Beer-Lambert Law:
\[
I = I_0 e^{-\alpha x}
\]
where:
- \( I_0 \) is the initial light intensity,
- \( I \) is the transmitted light intensity,
- \( \alpha \) is the absorption coefficient,
- \( x \) is the sample thickness.
We are given the following:
- For \( x = 1 \, \text{cm} \), \( I = 0.414 \, \text{mW/cm}^2 \),
- For \( x = 2 \, \text{cm} \), \( I = 0.186 \, \text{mW/cm}^2 \).
To calculate \( \alpha \), we first take the ratio of the two intensities:
\[
\frac{I_2}{I_1} = \frac{0.186}{0.414} = e^{-\alpha (2 - 1)}.
\]
Simplifying:
\[
0.449 = e^{-\alpha}.
\]
Taking the natural logarithm:
\[
\ln(0.449) = -\alpha,
\]
\[
\alpha = -\ln(0.449) \approx 0.804 \, \text{cm}^{-1}.
\]
Thus, the absorption coefficient is approximately \( 0.80 \, \text{cm}^{-1} \).