Photochemistry Core (Quantum Scale)
When photons strike a silver halide crystal (AgX), a photolytic reaction is triggered:
1.1 Photoelectron Excitation
$$ \text{AgX} + h\nu \xrightarrow{k_{\text{photo}}} \text{Ag}^+ + \text{e}^- + \text{X}^0 $$
Where:
- $h\nu$ is the photon energy ($\nu$ is frequency)
- $k_{\text{photo}}$ is the photochemical reaction rate constant, following the quantum efficiency model:
$$ k_{\text{photo}} = \eta \cdot \sigma_{\text{abs}} \cdot \Phi $$
- $\eta$: Quantum efficiency (≈0.6-0.9)
- $\sigma_{\text{abs}}$: Crystal absorption cross-section
- $\Phi$: Photon flux (photons/(cm²·s))
1.2 Latent Image Center Formation
Released electrons are trapped by silver ions, forming silver atom clusters:
$$ \text{Ag}^+ + \text{e}^- \xrightarrow{k_{\text{trap}}} \text{Ag}^0 $$
Critical Condition: A stable latent image center is formed when a single crystal surface accumulates 5-10 silver atoms:
$$ n_{\text{Ag}} \geq n_{\text{critical}} \approx 5-10 $$
This process can be modeled using a Poisson distribution:
$$ P(n_{\text{Ag}} \geq n_{\text{crit}}) = 1 - \sum_{k=0}^{n_{\text{crit}}-1} \frac{\lambda^k e^{-\lambda}}{k!} $$
Where $\lambda = \eta \cdot N_{\text{photons}}$ is the expected number of electrons.
Exposure and Density Mapping (Macro Scale)
2.1 Exposure Definition
$$ E = I \cdot t $$
- $I$: Irradiance (lux)
- $t$: Exposure time (s)
- $E$: Exposure (lux·s)
2.2 Optical Density
The ability of silver grains to block light after development is quantified by Optical Density $D$:
$$ D = \log_{10}\left(\frac{I_0}{I_t}\right) = -\log_{10}(T) $$
- $I_0$: Incident light intensity
- $I_t$: Transmitted light intensity
- $T = I_t/I_0$: Transmittance
Characteristic Curve (Hurter-Driffield Curve)
This is the core mathematical model of film imaging, describing the S-shaped relationship between $D$ and $\log_{10}E$:
3.1 Piecewise Linear Model (Engineering Simplification)
$$ D(\log E) = \begin{cases} D_{\text{min}} + \frac{\log E - \log E_{\text{toe}}}{\gamma_{\text{toe}}} & \text{Toe (Underexposed)} \ D_{\text{min}} + \gamma \cdot (\log E - \log E_0) & \text{Linear Region (Normal Exposure)} \ D_{\text{max}} - \frac{\log E_{\text{shoulder}} - \log E}{\gamma_{\text{shoulder}}} & \text{Shoulder (Overexposed)} \end{cases} $$
Key Parameters:
- $\gamma$: Contrast coefficient (slope of the linear region) $$ \gamma = \frac{\Delta D}{\Delta \log E} = \frac{D_2 - D_1}{\log E_2 - \log E_1} $$
- Dynamic Range: $\text{DR} = \log_{10}(E_{\text{max}}/E_{\text{min}}) \approx 2.0$ (corresponding to 100:1 brightness ratio)
3.2 Precise Error Function Model (Scientific Grade)
Analytical solution provided by Kodak technical documents:
$$ D(E) = \frac{D_0}{2}\left[1 + \text{erf}\left(X + \ln\frac{E - E_0}{E_g - E_0}\right)\right] $$
Where the error function is:
$$ \text{erf}(y) = \frac{1}{\sqrt{\pi}} \int_{-\infty}^{y} e^{-z^2} dz $$
Parameter meanings:
- $D_0$: Maximum saturation density
- $E_0$: Threshold exposure
- $E_g$: Sensitivity reference point
- $X$: Development condition correction term
Development Kinetics (Chemical Amplification)
Development amplifies latent image centers by $10^6$-$10^8$ times. Its rate equation:
4.1 First-Order Kinetics Model
$$ \frac{d[\text{Ag}]}{dt} = k_{\text{dev}} \cdot [\text{Dev}] \cdot [\text{Ag}^+] \cdot N_{\text{latent}} $$
- $[\text{Dev}]$: Developer concentration
- $N_{\text{latent}}$: Number of latent image centers (proportional to exposure)
4.2 Time-Temperature Compensation (Arrhenius Equation)
$$ k_{\text{dev}} = A \cdot e^{-E_a/(RT)} $$
- $E_a$: Activation energy (≈50-70 kJ/mol)
- $R$: Gas constant
- $T$: Absolute temperature (K)