CFRP Cryotanks Crack at Cryogenic Temperatures: A Resin Study That Targets the Root Cause

August 2025 Addcomposites 12 min read
CFRP cryotanks and cryogenic resin study

When carbon fibre-reinforced polymer (CFRP) replaces metal in a cryogenic tank, the carbon fibres are rarely the problem. The matrix is. At liquid-oxygen and liquid-hydrogen temperatures, conventional epoxy resins lose the small amount of molecular mobility that lets them tolerate strain, turn brittle, and crack between the fibres. Those matrix microcracks then link up into leak paths — the failure mode that has historically kept composite tanks out of the most demanding spaceflight roles.

A peer-reviewed, open-access study published in August 2025 in Polymers (MDPI) goes after exactly that root cause. A team from Zhejiang University's Institute of Advanced Equipment and Hydrogen Energy Institute set out to design an epoxy system that stays processable enough for wet filament winding and keeps usable toughness deep into cryogenic territory, then characterised both the neat resin and the resulting CFRP from room temperature down to 90 K.

The work is framed around onboard cryo-compressed hydrogen (CcH₂) storage vessels. But the underlying physics — matrix embrittlement, thermal-contraction mismatch, and the competition between cryogenic strengthening and thermal-stress damage — is the same physics that governs CFRP propellant tanks for launch vehicles and spacecraft. That overlap is what makes the paper worth a close read for anyone building cryogenic composite pressure structures.

A note on scope

Everything attributed below to "the paper," "the study," or "the authors" comes from Qi et al. Anything labelled Our perspective is Addcomposites' own analysis and does not represent a view, recommendation, or endorsement from the authors. Full citation and DOI are at the end.

What the Study Actually Did

The authors started from a standard bisphenol-A epoxy (DGEBA, grade E51) and co-modified it with two additives chosen to balance flexibility against stiffness: a polyetheramine (Huntsman T5000) and a cycloaliphatic epoxy, CY179. The system was cured with methyl nadic anhydride (MNA) and accelerated with DMP-30. By weight, the formulation ran 80 parts E51, 20 parts T5000, 20 parts CY179, 93 parts MNA, and 1 part DMP-30 (parts per hundred resin).

Ball-and-stick molecular models of the five resin components and the preparation flow of the modified epoxy.

Ball-and-stick molecular models of the five resin components — DGEBA base epoxy, CY179 cycloaliphatic epoxy, MNA hardener, DMP-30 accelerator, and T5000 polyetheramine — alongside the step-by-step preparation flow of the modified epoxy, from mixing in a heated three-necked flask through the staged oven cure and casting. Figure 1 from: Qi, L.; Wang, K.; Ge, Z.; Cao, Z.; Hu, P.; He, Y.; Yasin, S.; Shi, J. "Investigation of Cryogenic Mechanical Performance of Epoxy Resin and Carbon Fibre-Reinforced Polymer Composites for Cryo-Compressed Hydrogen Storage Onboard Gas Vessels." Polymers 2025, 17, 2296. https://doi.org/10.3390/polym17172296 — © 2025 by the authors. Licensed under CC BY 4.0 (https://creativecommons.org/licenses/by/4.0/).

The intent behind the polyetheramine is structural. The paper describes it reacting with the epoxy as the system cures, growing branched, pliable chains that spread through the finished network — in effect seeding soft pockets inside an otherwise rigid thermoset, an interpenetrating-network approach meant to absorb energy and blunt cracks rather than let them run.

Cross-sectional schematic of the vacuum-assisted resin infusion (VARI) setup.

Cross-sectional schematic of the vacuum-assisted resin infusion (VARI) setup, showing the vacuum pump, sealant, vacuum bag, carbon fibre layup, release cloth, diversion net, and heated mold, with the resin reservoir feeding in from the side. Figure 2 from: Qi, L.; Wang, K.; Ge, Z.; Cao, Z.; Hu, P.; He, Y.; Yasin, S.; Shi, J. "Investigation of Cryogenic Mechanical Performance of Epoxy Resin and Carbon Fibre-Reinforced Polymer Composites for Cryo-Compressed Hydrogen Storage Onboard Gas Vessels." Polymers 2025, 17, 2296. https://doi.org/10.3390/polym17172296 — © 2025 by the authors. Licensed under CC BY 4.0 (https://creativecommons.org/licenses/by/4.0/).

From Resin to Composite Coupons

To make the composite specimens, the team used vacuum-assisted resin infusion (VARI) with T700 unidirectional carbon fibre, producing both longitudinal (0°, fibre-aligned) and transverse (90°, across-the-fibre) coupons. They then ran tensile tests and coefficient-of-thermal-expansion (CTE) measurements at five temperatures — 300 K, 250 K, 200 K, 150 K, and 90 K — and examined every fracture surface under SEM.

Photographs of the cryogenic tensile testing setup.

Photographs of the cryogenic tensile testing setup — the servo-hydraulic testing machine, the cryogenic plate fixture, the liquid-nitrogen control system, and the cooled chamber with the mounted specimen, extensometer, and temperature sensor. Figure 3 from: Qi, L.; Wang, K.; Ge, Z.; Cao, Z.; Hu, P.; He, Y.; Yasin, S.; Shi, J. "Investigation of Cryogenic Mechanical Performance of Epoxy Resin and Carbon Fibre-Reinforced Polymer Composites for Cryo-Compressed Hydrogen Storage Onboard Gas Vessels." Polymers 2025, 17, 2296. https://doi.org/10.3390/polym17172296 — © 2025 by the authors. Licensed under CC BY 4.0 (https://creativecommons.org/licenses/by/4.0/).

A point worth flagging for relevance: the authors measured a fibre volume fraction of roughly 41% in their VARI laminates and reported this closely matched the ~43.6% they measured in actual wet-filament-wound vessel specimens, which is their argument that the coupon data transfers to real wound hardware.

Processing First: The Viscosity Window That Makes It Windable

A resin that performs beautifully at 90 K is useless if it cannot impregnate fibre during layup. So the authors characterised flow before they characterised strength.

The paper reports the modified system at roughly 800 mPa·s at room temperature, sitting under the ≤850 mPa·s ceiling commonly specified for wet filament winding, and dropping to about 100 mPa·s near 60 °C — low enough for thorough fibre wet-out before the exotherm kicks in and viscosity climbs sharply toward gelation. The curing window itself, extrapolated from differential scanning calorimetry, runs from about 72.9 °C onset to 210.9 °C, which the authors describe as broad enough to allow flow before crosslinking locks the network.

Resin Processing Characterisation

Viscosity vs. Temperature

Modified DGEBA / T5000 / CY179 system  ·  Qi et al., Polymers 2025

Viscosity curve
Usable processing window (25 – 120 °C)
Wet-winding threshold (850 mPa·s)
Gelation onset
Exotherm onset

From the DSC and rheology, the authors built a four-stage cure — a pre-cure hold, two primary crosslinking stages, and a post-cure above the peak exotherm temperature — to drive the network toward full conversion while managing the thermal stress that develops during cool-down.

Our perspective

This is the detail that should catch a process engineer's eye. The headline result is cryogenic toughness, but the enabling result is that ~800 mPa·s number. A system that hits cryogenic targets yet behaves like honey at the tow is a lab curiosity; a system that wets out cleanly on a winding head is a manufacturing input. The paper treats processability as a gating requirement rather than an afterthought, and that ordering is the right one.

The Neat Resin: Stronger and Stiffer as It Gets Colder

Tested on its own, the modified resin did what a well-designed cryogenic thermoset should do — it got stronger and stiffer as temperature fell, with the trade-off showing up as reduced elongation.

The paper reports tensile strength rising from 69.2 MPa at 300 K to about 122.6 MPa at 90 K — roughly a 77% gain — while elastic modulus climbed from 2,433 MPa to 6,802 MPa, an increase near 180%. Both followed an essentially linear dependence on temperature, with the authors fitting strength and modulus against temperature at correlation coefficients around 0.98.

Cryogenic Property Characterisation

Neat Modified Resin — Tensile Properties vs. Temperature

DGEBA / T5000 / CY179 system  ·  Qi et al., Polymers 2025, Table 3

Tensile Strength
300 K → 90 K  ·  +77%
300 K
69.2 MPa
250 K
83.9 MPa
200 K
92.1 MPa
150 K
103.8 MPa
90 K
122.6 MPa
Colder → stronger
Tensile Modulus
300 K → 90 K  ·  +180%
300 K
2433 MPa
250 K
3650 MPa
200 K
4631 MPa
150 K
5921 MPa
90 K
6802 MPa
Colder → stiffer

What stops this from being a simple "colder is better" story is what happens to ductility. Above ~200 K the resin still yields and deforms noticeably; below 150 K, the authors attribute the change to the polymer running out of the internal room its chains need to move — so instead of yielding, it breaks. That is the embrittlement trap the modification is designed to soften.

And it does soften it, according to the fracture analysis. SEM of the resin's fracture surfaces showed dimples — a signature of plastic deformation — at every temperature tested, broad and open when warm and compressed into flatter, plate-shaped features when cold, but never gone entirely. The authors attribute this partly to phase separation: the polyetheramine does not disperse perfectly, leaving a "soft phase / hard phase" morphology. Small soft domains act as pinning points that catch and redirect advancing cracks, and the surfaces show the resulting toughening behaviour — cracks that change direction, particles tearing loose from the matrix, and debonding at the fibre–resin interface. The authors are careful to note the limit of this: too high a density of phase-separated regions creates stress concentrations that can seed cracks instead of stopping them.

The Thermal-Mismatch Problem, Quantified

Before the composite results make sense, the CTE story has to be on the table — because the thermal mismatch between fibre and matrix is the source of the internal stress that drives cryogenic cracking.

The paper reports the carbon fibre as nearly thermally inert along its axis (axial CTE around −0.9 × 10⁻⁶/K) and modestly expansive across it (transverse CTE about 7.2 × 10⁻⁶/K). The resin, by contrast, moves on cooling by something close to ten times that amount. That gap is exactly why a wound or laid-up laminate develops residual stress on cooling: two bonded materials want to shrink by very different amounts.

Thermal Compatibility

CTE Comparison — Why the Matrix Drives Thermal Stress

Representative values  ·  Qi et al., Polymers 2025, Tables 2 & 6

0 14 28 42 56 ×10⁻⁶ /K
Carbon Fibre
Axial (∥ fibre) essentially inert
≈ −0.9 ×10⁻⁶ /K
Transverse (⊥ fibre)
≈ 7.2 ×10⁻⁶ /K

CFRP Laminate
CFRP-0° fibre-aligned, fibre-dominated
4 – 6 ×10⁻⁶ /K
CFRP-90° across fibre, matrix-dominated
30 – 42 ×10⁻⁶ /K

Neat Resin (120 – 275 K)
Modified DGEBA/T5000/CY179 temperature-dependent range
29 – 56 ×10⁻⁶ /K
⚠️
Larger CTE → more thermal contraction on cooling → greater internal stress at the fibre–matrix interface. The resin and off-axis plies contract up to 60× more than the axial fibre direction, driving the cryogenic failure modes in CFRP pressure vessels.

In the fibre direction, the composite's contraction is governed by the near-inert fibres, so the longitudinal CTE stayed low and barely changed with temperature. Across the fibres, the matrix dominates, so the transverse CTE was much higher — and it decreased as the resin stiffened on cooling. This asymmetry is the seed of the most important composite-level finding.

The Headline: 0° Barely Moves, 90° Transforms

When the authors tested the actual CFRP, the two fibre orientations behaved like almost different materials — and that contrast is the practical core of the paper.

Longitudinal (0°, load along the fibres). Properties were dominated by the carbon fibre, which the authors note is only minimally temperature-sensitive. From 300 K to 90 K, tensile strength rose only about 4.3% (1,928.9 → 2,010.4 MPa) and modulus about 7.7%, with elongation down slightly. Stable, predictable, fibre-controlled.

Transverse (90°, load across the fibres). Here the matrix and the interface carry the load, so the resin's cryogenic strengthening showed up directly. The paper reports transverse tensile strength up about 52.2% (43.1 → 65.6 MPa) and transverse modulus up about 82.4% (6,561 → 11,969 MPa) over the same span.

Cryogenic Property Gains by Fibre Orientation

Property Gain: 300 K → 90 K

CFRP laminate orientations  ·  Qi et al., Polymers 2025, Tables 7 & 9

Tensile Strength
longitudinal
+4.3%
Fibre-controlled — near flat
90° transverse
+52.2%
Matrix-dominated — strong gain
Tensile Modulus
longitudinal
+7.7%
Fibre-controlled  ·  non-monotonic response
90° transverse
+82.4%
Matrix-dominated — decisive gain
🔬
The matrix improvement is invisible along the fibre and decisive across it. The 90° direction is effectively a direct test of matrix behaviour — +52% in strength and +82% in modulus from 300 K to 90 K, versus single-digit gains in the fibre-aligned direction.

There is a subtlety in the longitudinal modulus that the simple percentage hides. Rather than rising monotonically, it climbed to a peak near 150 K and then dipped slightly. The paper reports it going from 95.8 GPa at 300 K up to 104.8 GPa at 150 K, then back down to 103.3 GPa at 90 K.

Non-Monotonic Cryogenic Response

CFRP-0° Longitudinal Modulus — Peak near 150 K

Qi et al., Polymers 2025, Table 7 / Figure 12b

📈
Rising leg · 300 K → 150 K
Better fibre–matrix bonding at low temperature shares load more effectively, driving the modulus upward.
⚠️
Falling leg · 150 K → 90 K
Accumulated thermal-stress microdamage offsets bonding gains, causing a slight drop back to 103.3 GPa.

The Two Competing Mechanisms

The authors explain all of this through a tug-of-war between two effects that both intensify as temperature drops.

Mechanism 1 — cryogenic strengthening. Resin and fibre both stiffen, and matrix contraction tightens the grip on the fibres ("encapsulation"), so the bond carries load better between the two. This pushes strength and modulus up.

Mechanism 2 — thermal-stress microdamage. The same contraction mismatch that improves encapsulation also builds internal stress, which can debond the interface and crack the matrix. This pulls properties down.

Cryogenic Deformation Mechanisms

Which Mechanism Wins?

Competing effects at low temperature — outcome depends on what carries the load

Mechanism 1
Strengthening
  • Stiffer resin matrix
  • Tighter interfacial bonding
  • More efficient load transfer
vs
Mechanism 2
Microdamage
  • Thermal-stress microcracking
  • Interfacial debonding
  • Accumulated damage on cooling
0° Longitudinal
Fibre-dominated — fibre carries the load
Mech 1 (small) Mech 2 (small)
Both mechanisms are small — the fibre dominates and is relatively insensitive to what the matrix does. Net result: nearly flat property gain (+4–8%), with Mech 2 overtaking just enough near 150 K to produce a slight modulus dip.

90° Transverse
Matrix-dominated — matrix + interface carry the load
Mech 1 (dominant) Mech 2 (minor)
Mech 1 dominates throughout — the matrix and interface are directly in the load path, so stiffening and improved bonding translate directly into property gains. Net result: a strong, roughly linear rise in strength (+52%) and modulus (+82%) from 300 K to 90 K. The 90° direction is the matrix test.

The fracture surfaces backed this up. In the 0° coupons, the authors saw failure driven by the fibres themselves snapping, with resin clinging to and linking the fibres. The 90° surfaces showed a mix of matrix cracking and interfacial debonding, with shear bands forming because resin trapped between fibres is too constrained to deform in simple tension. The telling detail: at colder temperatures, the broken surfaces carried more clinging resin and a coarser texture — evidence that the bond was getting stronger, not weaker, in the transverse direction, even as the count of microcracks climbed alongside it. That coexistence is the whole point: toughening does not eliminate thermal-stress damage; it tips the balance so strengthening wins.

Why This Matters for AFP and Filament-Wound Cryogenic Structures

Our perspective

The finding that lands hardest for a manufacturer is the orientation split. In a real wound vessel or tank, hoop and helical plies put the matrix and interface in the load path — the conditions that map onto the 90° coupon, where this resin showed its biggest gains. The directions most vulnerable to cryogenic matrix cracking are exactly the directions where the modification did the most work. For anyone designing winding patterns or AFP layups for cryogenic service, that is an argument for treating the resin system as a first-class design variable, not a fixed input.

The Addcomposites AFP head placing a carbon fibre course during automated fibre placement.

The Addcomposites AFP head placing a carbon fibre course during automated fibre placement. The same head also runs filament winding — switching between them is set in software, not new hardware.

One Cell, AFP and Filament Winding

It also reinforces a position we hold about process choice. The Addcomposites AFP head is configurable for both automated fibre placement and filament winding — switching between them is a software and materials decision in AddPath (toolpath planning and simulation) and AddWind (filament winding simulation), not a separate capital purchase. A resin characterised here for wet filament winding, at a viscosity our customers' processes can handle, sits naturally inside that flexibility. The same cell that lays AFP courses onto a mandrel can wind hoop and helical layers with a wet system in this viscosity class.

The cell winds hoop and helical carbon fibre onto a mandrel while the same layup is planned and simulated in AddPath.

The cell winds hoop and helical carbon fibre onto a mandrel while the same layup is planned and simulated in AddPath on the laptop. The choice between AFP and filament winding is made here, in software — not with new hardware. The same head winding hoop and helical carbon fibre layers onto a mandrel. A wet resin in the viscosity class characterised in this paper fits naturally into this process.

A few honest boundaries, because the marketing angle should not outrun the data:

  • The paper is about hydrogen storage vessels, not propellant tanks. The physics transfers cleanly — matrix embrittlement and CTE mismatch behave the same way regardless of what is inside the tank — but the authors did not test propellant-tank hardware, and nothing here should be read as their endorsement of any spaceflight application.
  • The tested floor is 90 K. That is close to liquid-oxygen service (~90 K). Liquid hydrogen sits near 20 K, below the range these tests cover. Extending the trends to 20 K is extrapolation on our part, not a measured result, and matrix behaviour can change in ways linear fits will not predict.
  • This is a wet-infusion / wound system. The authors fabricated coupons by VARI and validated against wound vessels. We are not claiming the paper proves out a prepreg AFP process; the relevance runs through the wet filament winding pathway and the shared physics.

Our perspective on the bigger picture

The value of work like this to an AFP or filament-winding operation is that it narrows the materials search. When a customer asks whether composite can replace metal in a cryogenic tank, the honest historical answer has been "the fibres can, but the matrix is a liability." Studies that quantify a processable resin's cryogenic behaviour — and explain why it behaves that way, mechanism by mechanism — are how that liability gets retired. Pairing a characterised resin system with deterministic toolpath and winding simulation is how a promising chemistry becomes a repeatable, qualifiable part.

What the Authors Flagged as Next Steps

The paper closes by pointing forward, not declaring the problem solved. The authors flag two open questions: how the balance of resin to fibre shapes the interface and the way the laminate expands and behaves in the cold, and — importantly for reusable hardware — how the material holds up across repeated cold cycles rather than a single cool-down. That last point matters: as the broader cryotank literature shows, it is repeated fill-and-drain cycling, not a single cold soak, that historically accumulates the microcrack networks responsible for leakage.

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Read the Research

This article summarises and comments on the following open-access paper. For the full methodology, figures, and data, read the original:

  1. Qi, L.; Wang, K.; Ge, Z.; Cao, Z.; Hu, P.; He, Y.; Yasin, S.; Shi, J. "Investigation of Cryogenic Mechanical Performance of Epoxy Resin and Carbon Fibre-Reinforced Polymer Composites for Cryo-Compressed Hydrogen Storage Onboard Gas Vessels." Polymers 2025, 17, 2296. https://doi.org/10.3390/polym17172296

© 2025 by the authors. Published by MDPI, Basel, Switzerland. This is an open-access article distributed under the terms of the Creative Commons Attribution (CC BY 4.0) license (https://creativecommons.org/licenses/by/4.0/).

Addcomposites is not affiliated with the authors or their institutions. References to NASA programs and other cryotank literature are drawn from publicly available technical reporting and are used here for context only.

Addcomposites automated fiber placement and filament winding
Pravin Luthada

Pravin Luthada

CEO & Co-founder, Addcomposites

About Author

As the author of the Addcomposites blog, Pravin Luthada's insights are forged from a distinguished career in advanced materials, beginning as a space scientist at the Indian Space Research Organisation (ISRO). During his tenure, he gained hands-on expertise in manufacturing composite components for satellites and launch vehicles, where he witnessed firsthand the prohibitive costs of traditional Automated Fiber Placement (AFP) systems. This experience became the driving force behind his entrepreneurial venture, Addcomposites Oy, which he co-founded and now leads as CEO. The company is dedicated to democratizing advanced manufacturing by developing patented, plug-and-play AFP toolheads that make automation accessible and affordable. This unique journey from designing space-grade hardware to leading a disruptive technology company provides Pravin with a comprehensive, real-world perspective that informs his writing on the future of the composites industry.