Find how the intensity of light decreases as it passes
Find how the intensity of light decreases as it passes through a homogeneous transparent medium, given that the intensity lost in a thin layer is proportional to both the intensity entering that layer and the layer's thickness.
Explanation of Method
The stated proportionality translates directly into a first-order separable differential equation for the intensity as a function of penetration depth; solving it with the initial intensity as the boundary condition gives the classic exponential attenuation (Beer–Lambert) law.
Step 1: Set up the differential equation
Let $I(x)$ be the intensity after traveling distance $x$ into the medium, and $\mu$ the (constant) absorption coefficient. The stated law is $-dI=\mu I\,dx$, i.e.
\[\frac{dI}{dx}=-\mu I.\]
Step 2: Separate and integrate
\[\frac{dI}{I}=-\mu\,dx\quad\Longrightarrow\quad \ln I=-\mu x+C.\]
Step 3: Apply the initial condition
At $x=0$, $I=I_0$, so $C=\ln I_0$, giving $\ln(I/I_0)=-\mu x$, i.e.
\[\boxed{I(x)=I_0e^{-\mu x}}\]
Step 4: Characteristic lengths
The half-thickness (depth at which intensity halves) solves $\tfrac12=e^{-\mu x_{1/2}}$:
\[x_{1/2}=\frac{\ln2}{\mu}\approx\frac{0.693}{\mu}.\]
The attenuation length (depth at which intensity falls to $1/e$) is simply $x_e=1/\mu$.
Step 5: Fraction absorbed and optical density
The fraction of light absorbed after distance $x$ is $1-e^{-\mu x}$. For a slab of thickness $L$, the transmission is $T=e^{-\mu L}$ and the optical density (absorbance) is $A=\log_{10}(1/T)=\mu L/\ln10\approx0.434\mu L$.
Result
Final answer:
\[\boxed{I(x)=I_0e^{-\mu x},\qquad x_{1/2}=\frac{\ln2}{\mu},\qquad x_e=\frac1\mu}\]