Lead-Tin Phase Diagram

Phase Diagram Of Lead And Tin

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The Lead-Tin Phase Diagram: A Practical Guide to Solder's Most Important Map

Ever wonder why solder behaves the way it does? Why it melts at a temperature that doesn't match either of its ingredients? The answer lives in a single chart that every materials science student eventually memorizes — and that most working engineers quietly forget.

The phase diagram of lead and tin is one of those deceptively simple-looking graphs that explains an enormous amount about how metals behave when you mix them. Because of that, it's the backbone of solder technology, and honestly, it's one of the best teaching tools in all of metallurgy. Not because it's exotic, but because it shows you — in one picture — how two metals interact across every possible combination of temperature and composition.

Here's the thing — most people glance at it, memorize the eutectic point for an exam, and move on. But if you actually understand what's happening in that diagram, you understand something fundamental about how alloys work. So let's dig in.


What Is the Lead-Tin Phase Diagram?

At its core, a phase diagram is a map. Even so, it tells you what phase (or phases) of matter a material exists in at any given temperature and composition. For the lead-tin system, that means plotting temperature on the vertical axis and composition (usually in weight percent of tin) on the horizontal axis.

The lead-tin diagram is what metallurgists call a binary eutectic system. Because of that, when the liquid cools, it doesn't always freeze into one uniform solid. That sounds technical, but the idea is straightforward: you've got two metals — lead (Pb) and tin (Sn) — that are completely miscible as liquids but only partially soluble in each other as solids. Sometimes it splits into two different solid phases, and the way that happens depends entirely on the ratio of lead to tin.

The Key Features

There are a few landmarks on this diagram you need to know:

  • Pure lead melts at 327.5°C. That's the left edge of the diagram.
  • Pure tin melts at 231.9°C. That's the right edge.
  • The eutectic point sits at 61.9 wt% tin and 183°C. This is the single most important point on the entire diagram.
  • Two solid phases exist: α (lead-rich, with a small amount of tin dissolved in it) and β (tin-rich, with a small amount of lead dissolved in it).
  • The solvus lines show how much of one element can dissolve in the other as temperature drops.

The α phase has an FCC crystal structure — that's lead's natural structure, and tin just sneaks into the lattice as a substitutional impurity. The β phase has a body-centered tetragonal (BCT) structure, which is tin's natural form, with lead atoms substituting in.


Why It Matters / Why People Care

So why does anyone care about this particular phase diagram? Because solder. That's the short version.

For decades — centuries, really — the lead-tin system has been the dominant alloy for soldering electronics, plumbing, and metalwork. Practically speaking, the eutectic composition (61. 9% Sn, 38.1% Pb) melts at a single, sharp temperature: 183°C. That said, that's lower than either pure metal. And that's not a coincidence — it's the whole point of a eutectic.

Here's why that matters in practice. A eutectic alloy does exactly that — it freezes at one temperature, with no mushy in-between zone. So when you're soldering a joint, you want the metal to go from liquid to solid quickly and cleanly. That means less chance of cold joints, less movement during solidification, and a cleaner microstructure.

Non-eutectic alloys — compositions away from the eutectic point — don't behave this way. Plus, if the joint moves during that window, you get a weak, grainy connection. Plus, they pass through a mushy zone where liquid and solid coexist. Real talk: this is why the exact composition of your solder matters more than most hobbyists realize.

But it's not just about solder. The lead-tin diagram is the textbook example of a eutectic system because it's clean, well-studied, and easy to understand. Learn this one, and you've got the conceptual framework for understanding dozens of other binary systems — from aluminum-silicon to silver-copper.


How It Works: Reading the Diagram

Let's walk through the diagram zone by zone. This is where the real understanding lives.

The Liquid Region

At high temperatures, everything is liquid. Consider this: above the liquidus line — the curved line connecting the melting points of pure lead and pure tin through the eutectic point — the alloy is fully molten regardless of composition. Simple enough.

The Liquid + Solid Regions

Between the liquidus and solidus lines, you're in a two-phase region. Also, this is the mushy zone I mentioned earlier. That's why depending on which side of the eutectic you're on, you'll have either liquid + α (on the lead-rich side) or liquid + β (on the tin-rich side). The alloy is partially solid and partially liquid, and the exact proportions depend on where you are in the region.

To figure out the proportions, you use the lever rule. It's a simple mass-balance calculation using a horizontal tie line at your temperature of interest. Plus, the fraction of each phase is proportional to the length of the tie line on the opposite side of your overall composition. It sounds confusing until you do it once — then it's obvious.

Continue exploring with our guides on impact factor journal of physical chemistry letters and how to cite in acs format.

The Eutectic Reaction

At exactly 61.9 wt% tin and 183°C, something special happens. The liquid transforms directly into a mixture of α and β phases simultaneously:

L (61.9% Sn) → α (19.2% Sn) + β (97.

This is the eutectic reaction. Because of that, the liquid doesn't freeze into one solid — it splits into two solids that grow together in a characteristic lamellar structure, alternating layers of α and β. This fine, alternating microstructure is what gives eutectic solder its strength and its sharp melting point.

The Solid Regions

Below the solidus (183°C for compositions near the eutectic), you're in solid territory. But it's not always simple:

  • α phase region: Lead-rich alloys with low tin content. Tin dissolves in the lead lattice up to

19.2 wt% at the eutectic temperature — after that, the excess tin precipitates as β phase. On cooling, this means primary α dendrites form first, then the remaining liquid hits the eutectic composition and transforms into that lamellar α+β mixture. The final microstructure shows those primary dendrites embedded in a eutectic matrix.

  • β phase region: Tin-rich alloys with low lead content. Lead dissolves in the tin lattice up to 2.5 wt% at the eutectic temperature. Same story in reverse: primary β dendrites first, then eutectic transformation.

  • The intermetallic layer: This is where the diagram meets reality. When molten solder contacts a copper pad, you don't just get dissolution — you get intermetallic compound (IMC) formation, primarily Cu₆Sn₅ and Cu₃Sn. These aren't on the simple Pb-Sn diagram because they involve a third element, but they dominate joint reliability. A thin, uniform IMC layer (1–3 μm) is good — it proves metallurgical bonding. Thick, scalloped, or fractured IMC? That's a reliability time bomb.


Why This Matters in Practice

Thermal Cycling Fatigue

The coefficient of thermal expansion (CTE) mismatch between solder (∼24 ppm/°C), copper (∼17 ppm/°C), and FR-4 (∼14 ppm/°C in-plane) means every temperature cycle stresses the joint. The eutectic's fine lamellar structure distributes strain better than coarse microstructures in off-eutectic alloys. But lead-free solders (SAC305: Sn-3.0Ag-0.5Cu) have different phase diagrams — primary β-Sn with Ag₃Sn and Cu₆Sn₅ particles — and their fatigue behavior is more complex. Understanding the Pb-Sn diagram gives you the mental model to approach those systems.

Reflow Profile Design

The mushy zone width dictates your reflow profile. For 63/37 eutectic, the liquidus and solidus meet at a point — zero mushy zone. You can ramp fast, peak sharp, and cool fast. For 60/40 (liquidus 188°C, solidus 183°C), you have a 5°C window where the joint is mechanically weak. Your profile must minimize time in that window, or vibration during conveyor transport will crack the semi-solid joint. This isn't theory — it's the difference between 10 ppm and 10,000 ppm defect rates.

Repair and Rework

Ever tried desoldering a joint with a cheap iron and watched the pad lift? You heated past the liquidus but the board acted as a heat sink, creating a thermal gradient. Part of the joint was liquid while the pad interface was still solid — shear forces did the rest. Knowing the diagram means you preheat the assembly to narrow that gradient. It means you understand why adding fresh eutectic solder to a lead-free joint creates a new, lower-melting ternary eutectic that helps component removal.

The Lead-Free Transition

The industry moved to SAC alloys not because they're better — they're not, mechanically — but because of RoHS. Their phase diagrams are ternary (Sn-Ag-Cu) with multiple eutectics and peritectics. The Sn-Ag binary has a eutectic at 3.5% Ag, 221°C. The Sn-Cu binary eutectic is 0.7% Cu, 227°C. SAC305 sits near the ternary eutectic (217°C) but solidifies with primary β-Sn dendrites first. That primary phase fraction changes with cooling rate. Fast cooling = finer dendrites = better fatigue life. The Pb-Sn diagram taught you to ask these questions.


The Bigger Picture

Phase diagrams are maps. The Pb-Sn diagram is the "Hello World" of metallurgy — simple enough to master completely, rich enough to teach every concept you'll need: liquidus, solidus, solvus, eutectic, terminal solid solubility, lever rule, microstructure evolution, non-equilibrium solidification.

Master this one diagram, and you can open ASM Handbook Volume 3, flip to any binary system — Al-Si for casting, Ni-Cr for superalloys, Fe-C for steel — and read it like a newspaper. You'll see the same topology, the same rules, the same lever rule. Only the numbers change.

The next time you hold a soldering iron, you're not just melting metal. Now, you're navigating a phase diagram in real time, choosing a path through composition-temperature space that determines whether that joint survives ten years or ten minutes. In real terms, the diagram doesn't care if you know it. The physics happens either way.

But you should know it.

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playontag

Staff writer at playontag.com. We publish practical guides and insights to help you stay informed and make better decisions.

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