Ch · Chemistry

Are Molten Metals Miscible With Each Other?

Published By the 9to5Science editorial team

At a glance

  1. 1. Check the metal pair

    Miscibility depends on the identities of both metals; some pairs form one liquid, while others separate.

  2. 2. Specify conditions

    Temperature and composition matter. A pair can be miscible at one temperature but separate into two liquid phases at another.

  3. 3. Read the phase diagram

    A liquid miscibility gap marks compositions and temperatures where two liquids are more stable than one uniform melt.

  4. 4. Distinguish liquid from solid

    Mixing in the molten state does not guarantee that the metals remain mixed after cooling.

Molten metals are not universally miscible. Some pairs form one uniform liquid over the full composition range; others separate into two liquid phases over part of that range. The answer depends on which metals you combine, their proportions, and the temperature. A pair that mixes as a liquid may also separate into different solid phases as it cools.

What miscibility means for molten metals

Two metals are miscible in the liquid state if they can form a single homogeneous liquid phase at the specified temperature and composition. In that liquid, atoms of both metals are interspersed, though the proportions need not be equal.

If the liquid is immiscible under those conditions, it separates into two liquids with different compositions—for example, one richer in the first metal and one richer in the second. These are still liquid phases, not necessarily pure metals. Different densities may make the phases settle into layers, but density is not what makes them thermodynamically separate.

A familiar example of liquid-phase immiscibility is the copper–lead system. Its phase diagram includes conditions where a molten Cu–Pb mixture separates into a copper-rich liquid and a lead-rich liquid. This does not mean every Cu–Pb composition is separated at every temperature: the phase diagram is needed to identify the relevant conditions.

Why some pairs mix and others separate

The balance is described by the Gibbs free energy of mixing. For a binary liquid, a useful expression is

ΔGmix=ΔHmix−TΔSmix,\Delta G_{\text{mix}} = \Delta H_{\text{mix}} - T\Delta S_{\text{mix}},

where ΔHmix\Delta H_{\text{mix}} is the enthalpy change on mixing, ΔSmix\Delta S_{\text{mix}} is the entropy change, and TT is the absolute temperature. Mixing is favored when the mixed state has lower Gibbs free energy than the alternative separated states.

The entropy of mixing generally favors a uniform liquid, and its contribution grows with temperature. But the enthalpy of mixing depends on how the unlike metal atoms interact compared with like atoms. If those interactions make mixing energetically unfavorable, a single liquid can become unstable and split into two liquids. A higher temperature often reduces the tendency to separate, but the exact phase boundaries must be determined for each metal pair.

For a binary system, the liquid phase diagram plots temperature against composition. Inside a liquid miscibility gap, the stable state is two liquids with different compositions. At a fixed temperature, a horizontal tie line across the gap gives the compositions of those two liquids; the overall composition determines their relative amounts.

Worked example: a simplified mixing model

A regular-solution model illustrates how temperature can change the result. For a hypothetical equimolar liquid, let the interaction parameter be Ω=20 kJ mol−1\Omega = 20\,\text{kJ mol}^{-1}. The model gives

ΔGmix=Ωx(1−x)+RT[xln⁡x+(1−x)ln⁡(1−x)],\Delta G_{\text{mix}} = \Omega x(1-x) + RT\left[x\ln x + (1-x)\ln(1-x)\right],

where xx is the mole fraction of one metal and R=0.008314 kJ mol−1K−1R = 0.008314\,\text{kJ mol}^{-1}\text{K}^{-1}. At equal proportions, x=0.5x=0.5.

At T=1000 KT=1000\,\text{K}, the enthalpy term is 20(0.5)(0.5)=5.00 kJ mol−120(0.5)(0.5)=5.00\,\text{kJ mol}^{-1}. The entropy term is RTln⁡(0.5)=−5.76 kJ mol−1RT\ln(0.5)=-5.76\,\text{kJ mol}^{-1}. Thus ΔGmix≈−0.76 kJ mol−1\Delta G_{\text{mix}}\approx-0.76\,\text{kJ mol}^{-1} relative to the unmixed pure liquids. At 500 K500\,\text{K}, the entropy term is about −2.88 kJ mol−1-2.88\,\text{kJ mol}^{-1}, giving ΔGmix≈+2.12 kJ mol−1\Delta G_{\text{mix}}\approx+2.12\,\text{kJ mol}^{-1} relative to those pure liquids.

This calculation shows how entropy can favor mixing more strongly at higher temperature. It is only an illustration: the sign at one composition relative to pure liquids does not by itself prove that a homogeneous liquid is stable. To establish stability, compare its free energy with that of possible mixtures of two liquids across compositions.

Do molten metals form alloys?

Yes. A liquid mixture of metals is commonly called a molten alloy or alloy melt. But “alloy” does not guarantee complete miscibility at every temperature or composition. On cooling, the melt may solidify as one solid solution, as multiple solid phases, or through other phase changes. Liquid miscibility and solid solubility are separate questions, so use the appropriate liquid or solid regions of the phase diagram.

Common mistakes

  • Assuming all metals mix because they are metals: metallic bonding does not make every metal pair mutually miscible.
  • Assuming a single answer without specifying temperature and composition: both can change the number and compositions of the phases.
  • Treating layering as the cause of immiscibility: density can make already separated liquids stratify, but phase stability determines whether they separate.
  • Inferring solid behavior from the melt: a uniform liquid can produce multiple solid phases on cooling, and a solid alloy may have limited solubility even when the liquid mixes well.

References

  1. ASM Handbook, Volume 3: Alloy Phase Diagrams
  2. Binary Alloy Phase Diagrams, edited by T. B. Massalski

Spotted an error? Send a correction. Read how we write and check articles in our editorial policy.