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ERB222 Chap.5 Magma Chamber Processes and Crystallisation

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Chapter 5 of 12 · ERB222

Magma Chamber Processes and Crystallisation

Where rising magma stops

Most magma never reaches the surface. Week 4 follows it from the source to storage, where it stalls at traps such as the Moho or the brittle to ductile transition, at neutral buoyancy, or where flow turns sideways into sills.

Beneath volcanoes such as Mount St Helens, storage zones sit at 5 to 15 km, and the crust makes room through floor sagging, doming, stoping, faulting and incremental sheet stacking.

How a stored magma solidifies

Crystallisation runs over roughly 200°C, so a chamber freezes from its walls inward through a solidification front: a suspension zone at the liquidus, a capture front below 25% crystals, a mush of 25 to 50% and a rigid crust above 50%.

Mineral densities decide whether crystals settle or, as plagioclase can, float.

Reading crystallisation on phase diagrams

Binary eutectics and the An-Di-Fo ternary show how the liquid moves away from each crystallising mineral, along cotectic valleys, to a eutectic where temperature stays fixed until a phase is used up.

Bowen's reaction series generalises this into continuous and discontinuous branches, but the lecture is clear about its limits as a recipe for granite.

In this chapter

What this chapter covers

  • 01

    Magma ascent and stalling

  • 02

    Storage depth and space making

  • 03

    Solidification fronts and mush

  • 04

    Crystal settling and flotation

  • 05

    Binary eutectic crystallisation

  • 06

    An-Di-Fo ternary paths

  • 07

    Continuous and discontinuous series

  • 08

    Limits of Bowen's reaction series

Worked example · free

Lever rule on the B-rich side of a model eutectic

Q [4 marks]. AskSia-authored practice. In a model binary, pure B melts at 1320°C and the eutectic lies at 1180°C and 40% A, with a straight liquidus. A melt of 25% A cools. Find its liquidus temperature, the liquid composition and the fraction of B crystals at 1215°C, and the solid fraction just above the eutectic. The allocation is an AskSia study aid, not a University marking scheme.
Cooling path for bulk X = 70% A.Cooling path for bulk X = 70% A. Temperature rises upward and composition runs from B at left to A at right; the red tie line at 1280°C joins liquid at 60% A to pure A crystals, and the bulk point divides it 25 to 75.118012801480LiquidA + liquidB + liquidA + B solidEX = 70wt% A (B at left, A at right)T (°C)
Cooling path for bulk X = 70% A. Temperature rises upward and composition runs from B at left to A at right; the red tie line at 1280°C joins liquid at 60% A to pure A crystals, and the bulk point divides it 25 to 75.
  • 1Liquidus on the B side: T = 1180 + 140(0.40 − 0.25)/0.40 = 1232.5°C, where B starts to crystallise.
  • 1Liquid at 1215°C: X = 0.40 − 0.40(1215 − 1180)/140 = 0.30 A.
  • 1Lever with crystals of pure B (0% A): fraction B = (0.30 − 0.25)/(0.30 − 0) = 0.167, about 17%.
  • 1Just above the eutectic: fraction B = (0.40 − 0.25)/0.40 = 0.375, so 37.5% is solid and 62.5% liquid freezes at 1180°C.
The liquidus is 1232.5°C; at 1215°C the liquid holds 30% A and about 17% of the system is B crystals; just above the eutectic 37.5% is solid.
Sia tip — Measure each lever arm from the bulk point to the phase on the opposite side; if your crystal fraction exceeds the value at the eutectic before you reach it, you have swapped the arms.
Glossary

Key terms

Solidification Front
The zone between liquidus and solidus at a cooling chamber margin, where melt progressively turns to crystals.
Mush Zone
The part of a solidification front holding roughly 25 to 50% crystals, between the capture front and the rigid crust.
Cotectic
A boundary between two phase fields on a phase diagram, a temperature valley along which two minerals crystallise together.
Continuous Reaction Series
The branch of Bowen's series in which one mineral, plagioclase, keeps crystallising while its composition shifts from Ca-rich toward Na and K.
FAQ

Magma Chamber Processes and Crystallisation FAQ

How deep are magma chambers under volcanoes?

Seismic and petrological studies beneath Mount St Helens and Long Valley place crustal storage zones at about 5 to 15 km. Storage concentrates at traps such as the Moho and the brittle to ductile transition, yet pressures recorded by pyroxene and amphibole show crystallisation can happen at many levels.

What is the difference between continuous and discontinuous crystallisation?

Continuous crystallisation belongs to solid-solution minerals such as olivine, pyroxene and plagioclase, whose compositions change gradually with the liquid. Discontinuous crystallisation involves minerals without solid solution that appear abruptly at a cotectic or eutectic, so the assemblage changes in discrete steps as temperature falls.

Why does temperature stay constant at a eutectic?

At the eutectic two solids and a liquid coexist, and it is the lowest temperature at which liquid can exist in that system. Cooling cannot continue until one of the three phases is used up, which in crystallisation is the last liquid, so the system holds its temperature while it freezes.

Study strategy

Exam move

Sketch the four-zone solidification front with its 25% and 50% crystal boundaries until you can label it from memory. Then practise lever-rule questions on a hand-drawn binary, writing the liquid composition before every lever, and trace two An-Di-Fo paths, one starting in each mineral field. Close by listing the five problems with Bowen's series without notes.

Working through Magma Chamber Processes and Crystallisation in ERB222? Sia is AskSia’s AI Science tutor — ask any ERB222 Magma Chamber Processes and Crystallisation question and get a clear, step-by-step explanation grounded in how ERB222 is taught and assessed. Read this chapter free, then take your hardest questions to Sia.

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