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A process engineer sizing a 1,200 °C tube furnace usually asks two questions before the purchase order goes out: what is the melting point of quartz, and what will the tube actually do once it is hot. The first answer is short — crystalline quartz melts somewhere between 1670 °C and 1713 °C, depending on which crystalline form and which measurement route is quoted. The second answer is the one that decides whether the furnace runs for three years or three months.
Here is the working answer we give customers: quartz glass does not fail at its melting point. It fails where it sags, devitrifies or crystallises, and for standard transparent fused quartz that point arrives between 1100 °C and 1200 °C in continuous service. The rest of this article explains that gap, because the gap is where every purchasing decision actually lives.
The 1670 °C figure describes crystalline quartz — the mineral, with an ordered lattice of SiO4 tetrahedra. Heating it is not a single clean event. The alpha-to-beta inversion at 573 °C is a structural flip that most furnace users never notice, because they work with glass rather than crystal. Higher up, above roughly 870 °C, the lattice begins converting toward tridymite and cristobalite, and cristobalite melts at about 1713 °C. That is why textbooks, handbooks and supplier datasheets quote anything between 1670 °C and 1713 °C for the same chemical formula without anyone being wrong.
Melt crystalline quartz and cool it quickly and you get fused quartz glass, an amorphous solid. Amorphous means no long-range order, which in turn means no sharp melting point. Instead of a melting line there is a viscosity curve, and engineers read four practical points off that curve.
For buyers the distinction is practical, not academic. A crystalline quartz part and a fused quartz part can carry identical SiO2 purity statements and behave completely differently in the same furnace. The crystal form expands sharply at the 573 °C inversion and can spall or crack; the glass form has no inversion, which is the entire reason transparent quartz tubes, quartz plates and quartz windows are made from fused material rather than sliced crystal. When a drawing calls for an optical window that must hold at 900 °C, the material being specified is glass, not crystal, and it should be ordered that way.
There is a second consequence that is easy to miss. Fused quartz is a melted product, so the melting point sets the ceiling for the manufacturing process itself, not only for the finished part. Electric fusion furnaces run well above 2000 °C at the arc to melt high-purity sand, and the tube drawing process that follows works the glass at around 2000 °C. By the time a tube reaches a customer, it has already been hotter than it will ever be in service — which is exactly why the as-supplied bubble class and OH content matter so much.
Rather than one temperature, transparent fused quartz is specified by three, and all of them sit far below the melting point. The values below are typical for standard transparent quartz glass; exact figures move a little with OH content and grade.
| Reference point | Typical value | What it means on the shop floor |
|---|---|---|
| Strain point | About 1075 °C | Above this, internal stress relaxes slowly and dimensions begin to drift over long holds. |
| Annealing point | About 1140 °C | Internal stress is relieved within minutes; used after flame working or forming. |
| Softening point | About 1665 °C | The glass starts to flow under its own weight; the practical end of load-bearing service. |
| Working point | Around 2000 °C | Viscosity low enough for drawing, bending and lampworking into manifolds or U-tubes. |
Read that table as a set of limits rather than trivia. If a plate has to keep its flatness after ten thermal cycles, hold it under the strain point; above that, stress relaxes and geometry moves. If a tube is going to be flame-worked into a manifold or a U-shape, the working point tells you how much it will move under its own weight while hot. Softening is where the material stops behaving like a solid component and starts behaving like a very stiff liquid.
A rule we repeat often: a transparent quartz tube suspended across 600 mm at 1150 °C will sag measurably within a few hundred hours, even though it sits roughly 500 °C below softening. Sag, not melting, is the failure mode most furnace builders actually run into.
Designers rarely choose quartz in isolation; it is usually weighed against alumina, borosilicate or graphite. The chart below puts the key numbers on one scale, using softening points for glasses because softening is the figure that behaves like a working limit in a real furnace.
Three things stand out when the numbers are side by side. First, the softening point of fused quartz glass sits within a few tens of degrees of the melting point of crystalline quartz, so the headline figure and the practical ceiling are closer than most people expect. Second, the gap between quartz and borosilicate 3.3 is over 800 °C, which is why laboratories keep borosilicate for ambient chemistry and move to quartz cuvettes, quartz digestion tubes and quartz beakers once a method needs 300 °C or a clean UV path. Third, thermal shock performance does not follow temperature ranking: quartz survives a water quench from red heat largely because its expansion is about 0.55 ppm/K, so the strain across a wall stays small even under a brutal gradient, while alumina at 8 ppm/K will not.
| Material | Melting or softening point | Expansion, ppm/K | Typical continuous use | Typical role |
|---|---|---|---|---|
| Fused quartz glass | Softens about 1665 °C | 0.55 | 1100–1200 °C | Furnace tubes, windows, crucibles, heaters |
| High-silica glass, 96 percent | Softens about 1530 °C | 0.8 | 900–1000 °C | Lower-cost furnace ware |
| Borosilicate 3.3 | Softens about 820 °C | 3.3 | 400–500 °C | Laboratory glassware, sight glasses |
| Soda-lime glass | Softens about 696 °C | 9.0 | Up to 300 °C | Lighting envelopes, general glazing |
| Alumina ceramic, 99 percent | Melts about 2054 °C | 8.0 | 1400–1500 °C | Insulators, setters, wear parts |
| Graphite | Sublimes above 3600 °C | 2 to 5 | 2000 °C plus, inert gas only | Susceptors, heating elements |
The graphite row explains a pattern you see in crystal-growing hot zones: graphite is used behind the quartz crucible, not instead of it. Graphite needs an inert or vacuum atmosphere, quartz does not, and quartz is transparent, which matters when a process engineer wants to see what is happening inside a reactor. Choosing between them is rarely about which one melts later.
Two quotations for what looks like an identical transparent quartz tube can differ by 30 percent, and the melting point is almost never the reason. Standard transparent grades are all specified in the same band. What moves is OH content, bubble class and trace metallic impurity, and those three change how the part behaves below softening.
OH content is the practical variable. Hydroxyl groups break up the silica network and lower viscosity, so a high-OH tube sags earlier at the same temperature than a low-OH tube of identical dimensions. The trade-off is not free: low-OH material holds shape better in a hot furnace but absorbs differently in the infrared, which matters for heaters and for infrared optical parts. That is the real reason a datasheet lists both a softening point and an OH figure.
Bubbles work the same way. A visible bubble string near the inner wall becomes a nucleation site for cristobalite growth, and cristobalite is the beginning of the milky patch that eventually flakes into the process chamber. Two tubes with the same softening point but different bubble classes will not have the same service life.
Once a part is inside a furnace, nobody is checking the melting point any more. The questions are whether the tube keeps its bore, whether a flange joint stays sealed after forty cycles, and how quickly the inner wall goes milky.
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At 1150 °C a transparent quartz tube is roughly 500 °C below softening yet still creeps under load. The mechanism is viscous flow at the support points and at any point where the wall carries weight. Practical countermeasures are unglamorous and effective: shorten the span between supports, rotate the tube between campaigns if the geometry allows, and specify heavy-wall sections where the tube must bridge a wide hot zone without intermediate support.
Above about 1150 °C, devitrification becomes the dominant ageing mode rather than sag. Surface contamination — fingerprints, alkaline dust, residues from cleaning agents, contact with certain refractory cements — catalyses cristobalite formation, and cristobalite grows as opaque white patches that eventually spall. Handling with clean gloves and storing tubes capped is not fussiness; it directly extends service life.
Solids behave differently from thin walls. A solid quartz rod used as a support or a fixture has more thermal mass and heats more slowly, which reduces the gradient across the part but increases the penalty for a badly controlled ramp. Quartz plates and discs used as windows, baffles or wafer carriers are usually limited by flatness rather than by strength, so the strain point becomes the operative ceiling: a plate that must stay flat should not be run above about 1075 °C for long holds.
For parts that must hold tight tolerances, precision-ground quartz is normally specified with the temperature history in mind, because grinding a part and then running it hot can release stress that was locked in during fabrication. A supplier who knows the intended service temperature will normally recommend an annealing step before final grinding.
Crucibles are the one application where the service temperature genuinely crowds the melting point. In Czochralski crystal growth, the silicon melt sits around 1420 to 1450 °C, and the inner wall of the crucible, in contact with that melt, runs hotter still. The outer wall touches a graphite susceptor that is itself above 1400 °C. For a few hundred hours the quartz wall is the hottest structural ceramic in the machine.
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At these temperatures the wall is above the strain point by several hundred degrees and it deforms. That is accepted, because a crucible is designed as a consumable with a known service window. What the industry manages instead is the progression: the inner surface slowly converts to cristobalite, the converted layer generates particles, and the mechanical strength of the wall falls as the conversion deepens. End of life is declared long before anything approaches melting.
Electronic-grade crucibles are built in layers for exactly this reason. A high-purity inner layer protects the melt from contamination, a bubble-containing intermediate layer provides thermal insulation and structural resilience, and an outer layer provides mechanical strength against the susceptor. Photovoltaic-grade crucibles follow the same logic with a shorter duty cycle, where cost per kilogram of silicon matters more than the last few percent of service life.
When buying, the questions that predict performance are not about the melting point of quartz. They are about bubble distribution, inner-surface purity, wall thickness tolerance and the specified thermal history the crucible has already seen during manufacture. A wholesaler or distributor handling large volumes will usually hold to a tighter wall tolerance than a general trader, because furnace operators index their susceptor geometry to that tolerance.
Optical quartz parts add a second constraint that most thermal parts do not have: whatever happens to the transmission curve after the part has been hot. A window that survives the temperature but loses deep-UV throughput is a failed specification.
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Far-UV optical quartz is the high-OH grade, transmitting well below 250 nm but with viscosity affected by that same hydroxyl content. UV-grade quartz sits in the middle, and infrared-grade quartz is deliberately low in OH so that the absorption band near 2.7 micrometres stays out of the working range. Each grade has essentially the same melting point; each behaves differently when a lamp housing reaches 800 °C.
Two thermal effects matter for optical parts. The first is stress birefringence: a window clamped between a hot flange and a cold frame develops a gradient, and the resulting stress changes polarisation. The second is more permanent — prolonged exposure to high temperature combined with UV flux can compact or solarise the material, shifting transmission slowly over a campaign. Neither is a melting problem, and neither will show up if a buyer only asks for the melting point.
Most quartz in the world never gets close to its limit. A carbon-fibre infrared heating tube holds a filament around 1100 °C inside an envelope that runs far cooler, and the envelope's job is transmission and mechanical protection rather than heat resistance. Milky or opaque quartz is often preferred there because it diffuses the emission and hides the filament, even though its transmission is lower than clear material.
Laboratory quartz ware is the same story with a different twist. A quartz digestion tube working at 250 °C with hot acid is nowhere near any thermal limit; its enemy is thermal shock during rinsing and handling, plus attack by hydrofluoric acid or hot concentrated alkali. Quartz beakers, cuvettes and evaporation dishes fail from handling and chemistry far more often than from temperature.
That makes the melting point of quartz almost irrelevant in these product families — and it makes delivery consistency, wall tolerance and surface finish the things worth negotiating. For a distributor or a laboratory supply wholesaler, the practical value of a manufacturer who publishes bubble class and OH data is that fewer units come back cracked after the first wash.
Everything below assumes transparent fused quartz of ordinary commercial grade. They are the checks that prevent most premature failures we see discussed in incoming enquiries.
Adding these six checks to a specification costs almost nothing at the drawing stage and can add months to a furnace campaign. The one that pays back fastest is usually the support spacing, because it is a geometry change rather than a material change.
Crystalline quartz melts between roughly 1670 °C and 1713 °C, which is about 3040 °F to 3115 °F. The range exists because different crystalline forms of SiO2 convert and melt at slightly different temperatures. Fused quartz glass does not have a true melting point; it softens around 1665 °C and flows gradually above that.
It softens. Because fused quartz is amorphous, it passes through a viscosity range rather than crossing a melting line. That is why a quartz tube can be bent at 2000 °C, drawn into capillary at similar temperatures, and still hold a load at 1100 °C.
Not reliably in air. Standard transparent grades are rated for roughly 1100 °C to 1200 °C continuous, with short excursions higher. Opaque and some specialty grades tolerate more, but sag and devitrification, not melting, set the limit. For sustained operation above 1200 °C, the support design and atmosphere usually need to change as well.
That is devitrification: amorphous silica converting to cristobalite, usually starting at a contaminated spot or at a bubble. It is accelerated by alkali, by handling residue and by higher temperature. Once a patch forms, it tends to grow and eventually spalls.
Only marginally, but it changes viscosity and therefore sag noticeably. Low-OH grades hold shape better in long hot holds, while high-OH grades are easier to work and transmit further into the deep UV.
Chemically yes, structurally no. Quartz is crystalline SiO2; fused silica or quartz glass is the same composition in an amorphous state, produced by melting and rapid cooling. Almost every transparent quartz window, tube and crucible in industrial use is the glass form.
For standard transparent material in air, plan on 1100 °C continuous and up to about 1300 °C for short excursions with good support and a clean surface. Low-OH grades and thicker walls shift those figures modestly, but they do not change the order of magnitude.
Give the peak temperature, the continuous temperature, the dwell time, the atmosphere, the support or clamping geometry, and any optical transmission requirement. Those five answers determine grade, OH level and wall thickness far more than the melting point does, and they let a supplier quote a part that will still be in one piece at the end of the campaign.
If a project sits anywhere between 1000 °C and 1300 °C, the sensible next step is to compare the intended duty against actual product pages rather than a generic materials table. The two most useful starting points are the tube range, where wall thickness and OH level drive everything, and the low-OH grades, where dimensional stability at temperature is the whole point.
Product references for high-temperature duty
A manufacturer working from its own furnace data will normally answer a temperature question with a grade recommendation rather than a single number, and that is the answer worth having. Melting points rarely lose a furnace campaign; a tube that sags two millimetres too far, or a window that goes cloudy in the wrong wavelength, does. Bring the peak temperature, the hold time and the atmosphere, and the number stops being trivia and starts being a specification.