HDT vs Vicat Softening Temperature: How to Read Both Numbers
Open almost any thermoplastics datasheet and you will find two numbers sitting next to each other under “thermal properties.” One is heat deflection temperature, HDT for short. The other is Vicat softening temperature, usually abbreviated VST. They are printed in adjacent cells, both in degrees Celsius, and people read them as two flavors of the same thing.
They are not the same thing, and treating them as synonyms is how parts end up sagging in service.
HDT asks: how hot can this loaded part get before it bends too far? Vicat asks: how hot can this surface get before something starts sinking into it? One is about structure holding load. The other is about a surface losing its nerve. Pick the wrong one for your decision and you can be off by 75 °C, which is not a rounding error.
This guide covers what each test does, why Vicat nearly always reads higher, how crystallinity decides the size of the gap, why glass fiber transforms one family of polymers and barely touches the other, and which number belongs in your specification.
The 60-second version
Both are short-term heat tests. They load the polymer in completely different ways.
HDT bends a bar. A specimen rests on two supports, gets a steady flexural load at the midpoint, and sits in a silicone oil bath warming at 120 °C/h until it deflects by a set amount. It simulates a structural part doing structural work. ISO 75 and ASTM D648 are the governing standards.
Vicat stabs a surface. A flat-tipped hardened steel needle with a 1 mm² contact area presses down under a fixed weight while the bath heats at 50 or 120 °C/h. When the needle has sunk 1 mm, you write down the temperature. It simulates surface softening. ISO 306 and ASTM D1525 cover it.
Because Vicat measures local penetration and HDT measures the deflection of an entire beam, Vicat comes out higher. For amorphous materials like polycarbonate the difference is modest, roughly 10 to 15 °C. For semi-crystalline ones it can be staggering. HDPE shows an HDT around 50 °C at 1.8 MPa and a Vicat near 125 °C.
Neither figure is a material property in the way density is. Both depend on load, heating rate, specimen shape, and how the part was molded. Neither one is your maximum service temperature.
HDT: what happens when you heat a loaded bar
Start with the definition. HDT is the temperature at which a standard bar deflects by a specified amount under a specified bending stress. A cleaner way to picture it: it is one point on the modulus-versus-temperature curve, the point where stiffness has dropped enough that the load wins.
The setup
The bar goes on two supports, gets loaded in the middle, and soaks in a silicone oil bath that climbs at 120 °C/h. Using a liquid bath rather than hot air removes variability in heat transfer, which is why the number is reproducible across labs.
Endpoints differ by standard:
- ISO 75 measures a deflection equal to a 0.20 % increase in outer fiber strain.
- ASTM D648 uses a flat 0.25 mm of deflection.
The load is set by choosing a stress level:
| Method | Flexural stress | Intended use | Typical materials |
| A | 1.80 MPa (ISO) / 1.82 MPa (ASTM) | High stress, rigid plastics | PC, PEEK, PA, PPS |
| B | 0.45 MPa (ISO) / 0.455 MPa (ASTM) | Low stress, flexible plastics | PP, PE, PTFE |
| C | 8.00 MPa (ISO only) | Very high stress, hard compounds | Hard rubber, heavily filled systems |
Datasheets usually quote Method A. Usually. Check anyway, because plenty of them do not say.
The load trap, which ruins more comparisons than anything else
Same polypropylene, two methods:
- Method A, 1.80 MPa: HDT about 57 °C
- Method B, 0.45 MPa: HDT about 99 °C
Forty-two degrees of separation from one polymer. Now imagine building a material shortlist by pulling whichever value each supplier printed. Your ranking would be fiction. There is no other single habit that damages material selection quite this efficiently.
ISO 75 against ASTM D648
The headline difference is orientation. ISO lays the specimen flat. ASTM stands it on edge.
| Detail | ISO 75 | ASTM D648 |
| Specimen | 80 × 10 × 4 mm | 127 × 12.7 × 6.4 mm |
| Orientation | Flatwise | Edgewise |
| Span | 64 ± 1 mm | 101.6 mm (A) / 100.0 mm (B) |
| Heating rate | 120 ± 10 °C/h | 2 ± 0.2 °C/min |
| Start temperature | Below 27 °C | Ambient |
| Endpoint | 0.20 % strain increase | 0.25 mm |
Edgewise changes the second moment of inertia, so the hanging weight differs to reach the same fiber stress. In practice the two standards land within 2 to 5 °C of each other, which most of us treat as equivalent. The variables that genuinely move the result are the load level, how much water the nylon has absorbed, and whether the part was annealed.
What HDT is not
It is not the temperature where softening begins. It is the temperature where deflection hits a target value under a target load. Those sentences describe different physical events. A polymer can be past its Tg and still post a healthy HDT if crystals or fibers are picking up the load.
It is also not creep data. The whole test is over in minutes. Anything expected to hold a continuous load at temperature for months needs creep and creep-rupture curves, and HDT will not substitute for them.
Vicat: one square millimeter under a needle
The Vicat test borders on crude, and that is the point. A hardened steel needle with a flat circular tip of 1 mm² sits on the specimen. A weight pushes down. The assembly warms in an oil bath. When penetration reaches 1 mm, record the temperature. Three moving parts, no bending rig, no strain calculation.
Four ways to run it
ISO 306 defines methods by combining load and heating rate:
| Method | Load (N) | Rate (°C/h) | When you use it |
| A50 | 10 | 50 | Slow and gentle. Best repeatability. |
| B50 | 50 | 50 | The default under ISO 10350 |
| A120 | 10 | 120 | Quick screening at low load |
| B120 | 50 | 120 | Quick screening at high load |
Two behaviors follow directly from the mechanics.
Heavier load means the needle gets there sooner, so B methods read lower than A methods on identical material. Faster heating means less time for the polymer to relax under the tip, so 120 °C/h results can come in up to 10 °C above their 50 °C/h counterparts.
Cross-supplier comparisons only make sense when the method matches. ISO 10350, the standard for collecting comparable plastics data, settles on B50: 50 N at 50 °C/h.
Requirements worth knowing
- Thickness between 3 and 6.5 mm, minimum 10 × 10 mm of surface.
- Molded bars or pieces cut from sheet and finished parts both work.
- Thin sheet can be stacked, three layers maximum, at least 3 mm total.
- Needle diameter 1.128 ± 0.008 mm, with vertical travel accurate to 0.02 mm.
- Minimum immersion depth 35 mm. Start at least 50 °C under the expected result.
- Temperature sensor within 12.5 mm of the needle tip.
- Two specimens minimum per condition, and rerun if they disagree by more than 2 °C.
The part where Vicat quietly beats HDT
HDT involves the full cross-section, so frozen-in molding stress gets involved too. Heat the bar, let that internal stress relax, and it contributes deflection that has nothing to do with heat resistance. The number drifts with processing history.
The needle touches almost nothing. Surrounding material stays rigid and clamps the loaded zone from three sides, so residual stress has little room to act. VST tracks the polymer itself rather than the mold. That is why it dominates incoming inspection even in shops where HDT governs the design, and why suppliers like it for certificates of analysis.
Side by side
| Aspect | HDT | Vicat (VST) |
| Loading | Three-point bending, distributed | Point load through a needle |
| Load | 0.45 to 1.80 MPa flexural | 10 to 50 N concentrated |
| Endpoint | 0.25 mm or 0.20 % strain | 1 mm penetration |
| Detects | Loss of stiffness in bulk | Surface softening |
| Residual stress | Affects the result | Barely matters |
| Relative size | Lower | 5 to 15 °C higher typically, far wider for semi-crystalline grades |
| Standards | ISO 75, ASTM D648, GB/T 1634 | ISO 306, ASTM D1525, GB/T 1633 |
| Use it for | Loaded structural parts | Processing windows, surface stability, QC |
So why is Vicat the bigger number?
The answer is constraint.
In bending, every fiber across the section carries load. Warm the bar and modulus falls everywhere at once. Softening in any layer drags the whole beam down, and there is nowhere to hide. Deflection shows up early.
Under the needle, only 1 mm² is being pushed, and everything around it is still cool and stiff. That surrounding material squeezes from three directions. To sink a full millimeter, the needle needs a decent volume of polymer to give way, not just a hot spot. More heat required, higher number recorded.
No mystery, no contradiction between the two tests. Just different amounts of material being asked to move. The effect magnifies whenever the polymer has internal structure resisting progressive heating, which takes us to crystallinity.
The trap worth committing to memory
With HDPE, PP, PBT and their relatives, gaps of 50 to 80 °C between the two values are routine rather than exceptional. HDPE sits near 50 °C on HDT at 1.8 MPa and near 125 °C on Vicat B50. Using one in place of the other is not a conservative shortcut. It is simply wrong, and the error is large enough to fail a product that looked perfectly specified on paper.
Crystallinity runs the whole show
Everything about the relationship between HDT, Vicat, Tg and Tm comes down to one question: does your polymer have crystals?
Amorphous: everything collapses at once
PC, PMMA, PSU, PEI, PAI and friends have a single thermal event. Cross Tg and the material goes from glassy to rubbery, with modulus falling three to four orders of magnitude. Both tests trigger near that drop because it is the only drop available.
Patterns to expect:
- HDT lands 5 to 15 °C under Tg, since deflection begins the moment modulus starts sliding.
- Vicat lands at or a little above Tg.
- The two values sit within about 10 °C of each other.
- Glass fiber does very little. Once the matrix goes rubbery, there is no crystalline framework left to help the fibers carry a bending load.
Polycarbonate spells it out: Tg near 145 °C, HDT about 135 °C, Vicat about 150 °C.
Semi-crystalline: a plateau held up by crystals
PA, POM, PP, PBT, PEEK, PPS and PET have two transitions. Amorphous regions soften at Tg, but the crystals stay intact and keep working as scaffolding. Modulus drops and then flattens. Somewhere across that plateau the remaining stiffness finally falls under the test threshold.
The progression:
- Tg arrives, amorphous regions soften, modulus declines but remains real
- Plateau where HDT and Vicat live, with crystals carrying the load
- Tm arrives, crystals melt, stiffness disappears
What that produces:
- HDT somewhere between Tg and Tm, exact position set by how much crystallinity there is.
- Vicat typically 20 to 80 °C above HDT, since a needle needs some crystal softening too.
- Enormous glass fiber response.
- Higher crystallinity pushes both numbers toward Tm.
PEEK is the clean example. Tg of 143 °C, Tm of 341 °C. Unfilled, it manages an HDT near 160 °C, barely above Tg, thanks to something like 30 to 35 % crystallinity. Add 30 % glass fiber and HDT reaches about 315 °C. Almost to the melting point, from a resin whose Tg is 143 °C.
If you remember one line, make it this one. Amorphous: HDT ≈ Vicat ≈ Tg. Semi-crystalline: Tg < HDT < Vicat < Tm. That explains why PC’s pair nearly overlap while PP’s sit 30 to 50 °C apart.
Glass fiber: spectacular in one case, nearly useless in the other
This asymmetry deserves more attention than it gets, and it has cost people real money.
Semi-crystalline grades make a jump toward Tm
PA66 has a dry Tg around 50 °C and melts near 260 °C. Unfilled, its HDT is roughly 85 °C. Add 30 % glass fiber and HDT reaches about 250 °C. That is a 165 °C gain, moving the material from “slightly better than Tg” to “almost at Tm.”
PA6 tells the same story, with published figures at 1.82 MPa:
- Unfilled: HDT 65 °C, modulus 2.81 GPa
- 14 % glass fiber: HDT 200 °C, modulus 4.46 GPa
- 33 % glass fiber: HDT 210 °C, modulus 7.87 GPa
Note what did not move. Tg goes from about 65 to 70 °C. The crystals do not change. What changes is load transfer: past Tg the softened matrix hands the work to the fibers, which stay rigid all the way up to melting. In PA, PP and PBT, 10 wt % of short glass fiber is often enough to push HDT close to Tm.
Amorphous grades shrug
- Unfilled PC: HDT about 135 °C at 1.8 MPa
- 30 % glass-filled PC: HDT about 145 to 150 °C
Ten or fifteen degrees for a third of the part weight in fiber. The reason traces back to the missing plateau. Above Tg there is nothing to keep the fibers working as a load path, so the section deflects as a unit. Stiff fibers floating in a rubbery matrix cannot prevent whole-beam bending.
If higher heat resistance is what you need from PC, switching to a higher-Tg resin gets you there. Loading it with fiber mostly gets you a higher price per kilo.
Aspect ratio sets the ceiling
The rule extends past glass fiber to every filler:
| Filler | Aspect ratio | Effect on HDT |
| Glass bead, calcium carbonate | ~1, spherical | Minimal |
| Talc, kaolin | 10 to 40:1 | Moderate |
| Wollastonite, wet-ground mica | 10 to 50:1 | Good |
| Chopped glass fiber, nanoclay | 50 to 200:1 | Strong |
| Carbon fiber, aramid fiber | 100 to 500:1 | Strongest |
Screening data across common engineering plastics
Use this for shortlisting. Do not use it for design.
| Material | Type | Tg (°C) | Tm (°C) | HDT @ 1.8 MPa (°C) | Vicat B50 (°C) |
| HDPE | Semi-crystalline | −110 | 135 | ~50 | ~125 |
| PP | Semi-crystalline | −10 | 165 | ~57 | ~90 |
| PP + 30% GF | Reinforced semi-crystalline | −10 | 165 | ~150 | ~160 |
| Rigid PVC | Amorphous | 80 | n/a | ~70 | ~85 |
| PS (GPPS) | Amorphous | 100 | n/a | ~85 | ~95 |
| PMMA | Amorphous | 105 | n/a | ~95 | ~110 |
| ABS | Amorphous | 105 | n/a | ~95 | ~100 |
| PET | Semi-crystalline | 75 | 255 | ~80 | ~170 |
| PET + 30% GF | Reinforced semi-crystalline | 75 | 255 | ~230 | ~250 |
| PBT | Semi-crystalline | 45 | 225 | ~60 | ~165 |
| PBT + 30% GF | Reinforced semi-crystalline | 45 | 225 | ~210 | ~220 |
| POM (copolymer) | Semi-crystalline | −60 | 175 | ~110 | ~150 |
| PA66 (dry) | Semi-crystalline | 50 | 260 | ~85 | ~240 |
| PA66 + 30% GF | Reinforced semi-crystalline | 50 | 260 | ~250 | ~255 |
| PC | Amorphous | 145 | n/a | ~135 | ~150 |
| PC + 30% GF | Reinforced amorphous | 145 | n/a | ~148 | ~155 |
| PSU | Amorphous | 187 | n/a | ~175 | ~188 |
| PEI | Amorphous | 217 | n/a | ~200 | ~215 |
| PPSU | Amorphous | 220 | n/a | ~205 | ~218 |
| PVDF | Semi-crystalline | −35 | 171 | ~112 | ~155 |
| PTFE | Semi-crystalline | −97 | 327 | ~55 | ~110 |
| PPS | Semi-crystalline | 90 | 280 | ~135 | ~200 |
| PPS + 40% GF | Reinforced semi-crystalline | 90 | 280 | ~260 | ~270 |
| PEEK | Semi-crystalline | 143 | 341 | ~160 | ~250 |
| PEEK + 30% GF | Reinforced semi-crystalline | 143 | 341 | ~315 | ~330 |
| PEEK + 30% CF | Reinforced semi-crystalline | 143 | 341 | ~315 | ~340 |
| PAI | Amorphous | 275 | n/a | ~275 | n/a |
| PI | Amorphous | 360 | n/a | ~360 | n/a |
Three things this table gives away
The semi-crystalline rows have wide gaps. PA66 reads 85 °C against 240 °C. PC reads 135 against 150.
Glass fiber gains are wildly uneven between families. PA66 gains 165 °C. PC gains about 13.
PTFE needs a warning label. Continuous-use temperature of 260 °C, HDT of around 55 °C. It loves heat and hates load. Nothing about those two facts contradicts, but put PTFE into a hot load-bearing job on the strength of its reputation and it will creep into failure.
Which one does your application need
HDT, when something is carrying load
Go to HDT when:
- The part holds sustained mechanical load at temperature, whether bending, compression or vibration.
- You want a short-term ceiling for structural service temperature.
- The application is under-hood automotive, an electrical enclosure, a loaded bracket, or comparable.
- You are verifying batch-to-batch structural heat performance in QC.
Typical cases: glass-filled PA intake manifolds, PC/ABS appliance housings, PBT and LCP connectors, PEEK and PPS structural components.
Vicat, when the surface is the concern
Vicat fits when:
- Heat arrives without meaningful load, but shape has to hold.
- You are setting a demolding window. It belongs comfortably below VST.
- You are running incoming inspection, where immunity to residual stress pays off.
- Thin walls, films and coatings are what you are judging.
Typical cases: hot-water dimensional stability in PVC and CPVC pipe, where specifications such as IS 4984 call for VST of at least 125 °C; interior trim baking in a parked car; hot-fill packaging; cable insulation.
Four cautions
HDT is not your service ceiling. Real parts face dynamic loading, years of thermal aging, and whatever chemicals are in the neighborhood. For amorphous polymers especially, take 20 to 40 °C off the HDT as a starting figure for continuous use, then confirm against long-term data such as the UL 746B Relative Temperature Index.
Annealing helps. Fast cooling during molding locks in stress and holds crystallinity down, and both suppress measured HDT. Heat above Tg but below Tm, cool slowly, and you relieve the stress while growing crystals. HDT rises, dimensional stability improves.
Nylon drinks water. Absorbed moisture plasticizes the amorphous phase and pulls Tg down with it. Dry-as-molded PA66 sits around 85 °C. Conditioned to equilibrium humidity it can fall to roughly 60 °C. Published values are almost always dry, so unless you can guarantee the part stays dry, design for the conditioned state.
Stop substituting one for the other. Semi-crystalline grades can differ by 50 to 80 °C between the two tests. Ask for both on every datasheet you receive.
Standards reference
| Property | International | US | China |
| HDT | ISO 75-1/2/3 | ASTM D648 | GB/T 1634 |
| Vicat | ISO 306 | ASTM D1525 | GB/T 1633 |
One machine covers both tests. Swap the loading head, change the weights, pick your method, and start the bath. Sharing the frame and the heating system is why so many labs quote them together. Current testers carry two to six stations, so a batch runs in a single cycle.
Where this leaves you
Two tests, two failure modes, two questions. HDT cares whether a loaded part still resists deflection. Vicat cares whether a hot surface still resists penetration. Neither tells you a safe long-term operating temperature by itself, and neither can stand in for the other.
Work backward from the part. Loaded at temperature? HDT at the right stress level is your figure, supported by creep data if the loading never stops. Worried about surface deformation, demolding, or batch verification? Vicat, with its method stated alongside. Then check amorphous versus semi-crystalline, because that decides how wide the gap should be and whether throwing glass fiber at the problem will accomplish anything.
Reading these numbers off a datasheet takes about a minute. Knowing which one applies takes slightly longer, and it is the part that actually matters.
Next steps worth taking:
- Shortlist on UL 746B RTI values rather than HDT when the design has to survive years of heat.
- Ask every supplier for Method A and Method B HDT, plus the Vicat method, before comparing quotes.
- For nylon and other hygroscopic grades, request conditioned-state properties, not just dry-as-molded.


