Alloy Junction 1952 Dissolve Germanium Locally
# Dissolve Germanium Locally: Approaching Step Eleven's Ceiling in Real Time
Step eleven's phase-diagram equation set a hard ceiling on how much germanium a given pellet mass could ever dissolve — but a ceiling is a thermodynamic limit, not a schedule, and this step is where the actual dissolving happens, governed by how fast germanium atoms can diffuse into the liquid indium rather than by how much the liquid could theoretically hold. Under each disk, a thin boundary layer of molten indium-germanium alloy forms at the interface and grows outward as dissolution proceeds, with the local germanium concentration climbing toward step eleven's equilibrium ceiling but never instantly reaching it. How close this step actually gets, in the time the schedule allows, depends on genuine mass-transport kinetics.
## 1. Dissolution Depth Grows With the Square Root of Time
The depth of germanium actually dissolved at time $t$ scales with the square root of elapsed time, scaled by the diffusion coefficient of germanium in liquid indium — the same square-root-of-time mathematical form that governed step nineteen's oxide growth and step twenty's thermal penetration, now describing mass transport instead of heat or oxidation. This is why dissolution depth isn't simply "however much the phase diagram allows" the instant melting occurs: it's a quantity that climbs continuously through the hold, approaching but never instantly reaching step eleven's ceiling, which means the scheduled hold time is doing real, measurable work rather than just waiting for an already-finished process to be declared complete.
## 2. Real Diagram: A Growing Alloy Layer, Not a Step Change
## 3. Step Twenty's Timing Lag Becomes a Real Depth Mismatch Here
Because dissolution depth follows a square-root law rather than a linear one, the small timing offset step twenty's thermal lag introduced between the two faces doesn't simply shift both curves by the same amount — differentiating the square-root relationship shows that a given $\Delta t_{\text{lag}}$ produces a depth mismatch $\Delta x$ that depends on how far along the dissolution process already is, meaning the consequence of an early-process timing error actually shrinks as the hold continues, since the square-root curve flattens with time. This is the first point in the process where step twenty's lag stops being an abstract timing concern and becomes an actual, calculable difference between $x_E$ and $x_C$ in step six's governing relationship.
## Dissolve Germanium Locally's Place in the Process Lineage
Dissolving germanium locally is step twenty-two of RCA's forty-two-step alloy-junction manufacturing sequence — immediately after both faces were wetted, and before the furnace schedule actively controls how far this dissolution is allowed to proceed. It is the step that converts step eleven's thermodynamic ceiling into a real, time-dependent process, governed by diffusion rather than instantaneous equilibrium, and it is the first point where step twenty's thermal lag becomes a calculable depth difference between the two junctions rather than a timing concern alone. Step twenty-three, controlling alloy penetration, picks up exactly where this step's growing dissolution front leaves off.