IG-110 isotropic graphite IG-110
C (carbon
Also known as IG-110
IG-110 is a fine-grained, isostatically pressed graphite made by Toyo Tanso and qualified by Oak Ridge National Laboratory (ORNL) as a candidate material for a high-temperature gas-cooled reactor.
Evidence level
2 of 5
Lab-measured
- 0Predicted only. No one has made it, or no measurement exists.
- 1Calculated. Only calculated or predicted values from sources.
- 2Lab-measured. Measured properties with their conditions stated.
- 3Space-relevant tests. Measured in conditions relevant to space, such as vacuum or atomic oxygen.
- 4Ground-qualified. Qualified for an application on the ground.
- 5Flown or field-proven. Flight or field results exist.
Density
1.77 g/cm³
Grain size
20 µm
Strength
34 MPa
Heat conduction
129 W/m/K
Oxidation in air
195 kJ/mol
Recipe, share of the weight
- C not statedCarbon filler
- not statedBinder carbon
- not statedPores
Best for
Reference nuclear graphite where ORNL baseline and irradiation data for the grade matter, such as reactor-core qualification studies
Weakest at
Irradiation and air oxidation: thermal conductivity falls sharply after neutron irradiation, and the graphite oxidizes in air at high temperature
Risk at a glance
- People Low. No IG-110 hazard data found; nearest is carbon
- If it fails High. Oxidation of hot graphite in air
- Corrosion Moderate. In air, IG-110 oxidizes, and the rate rises steeply with temperature.
Quick facts: IG-110
| Property | Value | Basis |
|---|---|---|
| Density | 1.76 to 1.77 g/cm³ | 2 sourced values across conditions |
| Tensile strength | 14.9 MPa | 1 sourced value |
| Young's modulus | 8.77 to 9.7 GPa | 3 sourced values across conditions |
| Thermal conductivity | 2.8 to 130 W/m/K | 3 sourced values across conditions |
| Thermal expansion (CTE) | 4.2 to 4.5 ppm/K | 2 sourced values across conditions |
What is the density of IG-110 isotropic graphite?
IG-110 isotropic graphite has a density of 1.76 to 1.77 g/cm³. The range covers 2 sourced values across the tempers, forms and test conditions the sources report; room-temperature values are used where a source states a temperature.
What is the thermal conductivity of IG-110 isotropic graphite?
IG-110 isotropic graphite has a thermal conductivity of 2.8 to 130 W/m/K. The range covers 3 sourced values across the tempers, forms and test conditions the sources report; room-temperature values are used where a source states a temperature.
What is the coefficient of thermal expansion of IG-110 isotropic graphite?
IG-110 isotropic graphite has a coefficient of thermal expansion of 4.2 to 4.5 ppm/K. The range covers 2 sourced values across the tempers, forms and test conditions the sources report; room-temperature values are used where a source states a temperature.
What is the tensile strength of IG-110 isotropic graphite?
IG-110 isotropic graphite has a tensile strength of 14.9 MPa. The source and test conditions are listed in the properties table on this page.
What is the Young's modulus of IG-110 isotropic graphite?
IG-110 isotropic graphite has a Young's modulus of 8.77 to 9.7 GPa. The range covers 3 sourced values across the tempers, forms and test conditions the sources report; room-temperature values are used where a source states a temperature.
What is IG-110 isotropic graphite used for?
Uses recorded in the sources include Core graphite structures in a high-temperature gas-cooled reactor (candidate material, not a deployed use); Semiconductor manufacturing parts made from isotropic graphite (the industry is named; IG-110 is not named).
Why it exists
IG-110 is an isotropic nuclear graphite made by Toyo Tanso. Isotropic means its properties are nearly the same in every direction. ORNL and Toyo Tanso ran a joint program to qualify it for a Generation-IV high temperature gas-cooled reactor. The program measured its baseline properties and how neutron irradiation changes them, and the results are published in ORNL reports.
Where it's used
Reactor core candidate
ORNL and Toyo Tanso qualified IG-110 as a candidate material for a Generation-IV high temperature gas-cooled reactor. The sources we hold describe this as a qualification role, not a deployed use.
Semiconductor industry
Toyo Tanso names the semiconductor industry as a user of its isotropic graphite. Its page does not name IG-110 in that list, so this is an industry-level claim.
Recipe
C (carbon; synthetic graphite made from petroleum-based carbon materials)
IG-110 is a synthetic graphite made from petroleum-based carbon materials and formed by isostatic pressing. ORNL describes nuclear graphite as a composite of filler, binder and pores, and says the vendor's process details are proprietary.
| Ingredient | Share of the weight | What it does |
|---|---|---|
| Carbon filler C | not stated | Carbon particles from a petroleum-based coke that form most of the graphite skeleton |
| Binder carbon | not stated | Carbon that binds the filler together after forming, baking and graphitization |
| Pores | not stated | Open and closed voids that set the density and strength of the finished block |
Weight shares are as printed in the sources.
What it can do
Density
1.77 g/cm³
measured
ORNL measured a bulk density of 1.77 g/cm3 before irradiation, so one cubic centimetre of the graphite weighs about 1.77 grams.
Grain size
20 µm
measured
The average grain size is 20 µm, printed in ORNL's 2022 review. This is the finest of the three nuclear graphites that review compares.
Strength
34 MPa
measured
Flexural strength is 34 MPa in the axial direction and 36 MPa in the transverse direction, before irradiation, in ORNL's 2018 report.
Heat conduction
129 W/m/K
measured
Thermal conductivity at 25 °C is 129 W/m/K in the axial direction before irradiation. After irradiation, one specimen read 2.80 W/m/K.
Oxidation in air
195 kJ/mol
measured
Air oxidation has an activation energy of 195 kJ/mol in one data set and 187 kJ/mol in another, both printed in ORNL's 2022 review.
How it compares
Among the three nuclear graphites that ORNL compares in its 2022 review, IG-110 has by far the finest average grain. PCEA is extruded and NBG-18 is vibrationally molded, while IG-110 is isostatically pressed. The forming method and the fine grain are the two features that separate IG-110 from the other two grades in that review.
The same measurements for each material, so you can compare them. Each row names the key condition under the value; the full conditions and methods are in the numbered notes under Technical details. Compare every grade in the family.
| Measurement | IG-110 |
|---|---|
| Capacity and energy | |
| Activation energy for air oxidation, Smith data set | 195 kJ/mol20 |
| Activation energy for air oxidation, Fuller data set | 187 kJ/mol21 |
| Activation energy for air oxidation, Chi data set | 169 kJ/mol22 |
| Thermal behavior and safety | |
| Thermal conductivity at 25 °C, TD4 specimens, axial | 129 W/m/K12 |
| Thermal conductivity at 25 °C, TD4 specimens, transverse | 130 W/m/K13 |
| Thermal conductivity at 500 °C, TD4 specimens, axial | 73 W/m/K14 |
| Thermal conductivity at 500 °C, TD4 specimens, transverse | 77 W/m/K15 |
| Thermal conductivity after neutron irradiation, sample T11T15 | 2.8 W/m/K23 |
| Lifetime and stability | |
| Volume change after neutron irradiation, sample T10T06 | -7.39 %24 |
| Physical and electrical | |
| Bulk density, pre-irradiation specimens | 1.77 g/cm³1 |
| Bulk density, ORNL 2022 Table 1 | 1.761 g/cm³2 |
| Other measurements | |
| Dynamic Young's modulus, MB specimens, axial | 9.1 GPa3 |
| Dynamic Young's modulus, MB specimens, transverse | 9.7 GPa4 |
| Compression strength, CRS specimens, axial | 77 MPa5 |
| Compression strength, CRS specimens, transverse | 77 MPa6 |
| 4-point flexural strength, MB specimens, axial | 34 MPa7 |
| 4-point flexural strength, MB specimens, transverse | 36 MPa8 |
| Mean coefficient of thermal expansion at 500 °C, MB axial | 4.5 ppm/K9 |
| Mean coefficient of thermal expansion at 500 °C, MB transverse | 4.2 ppm/K10 |
| Isotropy ratio of thermal expansion | 1.057 -11 |
| Average grain size | 20 µm16 |
| Ash contentPrinted by ORNL in the general properties table | < 10 ppm |
| Tensile strength, ORNL 2022 Table 1 | 14.9 MPa17 |
| Compressive strength, ORNL 2022 Table 1 | 73.44 MPa18 |
| Dynamic Young's modulus, ORNL 2022 Table 1Printed by ORNL in the general properties table | 8.767 GPa19 |
| Poisson's ratioPrinted by ORNL in the general properties table | 0.157 - |
Why choose it, and why not
Good for
- Reference data. ORNL measured baseline values for IG-110 in two reports and one 2022 review.
- Reactor-core qualification work, where irradiation data for this grade already exist.
- Parts that need similar strength in both directions: the flexural strength is 34 MPa axially and 36 MPa transversely.
Watch out for
- Thermal conductivity falls sharply after irradiation. One specimen dropped from 129 W/m/K to 2.80 W/m/K.
- Hot IG-110 oxidizes in air. The 2022 review reports activation energies of 195 kJ/mol and 187 kJ/mol.
- Density differs between ORNL sources: 1.77 g/cm3 in the 2018 report and 1.761 g/cm3 in the 2022 review.
IG-110 is a well-documented nuclear graphite with ORNL baseline and irradiation data. Its weak points are irradiation-driven conductivity loss and oxidation in air at high temperature.
Technical details
For scientists and researchers. Everything above comes from the record below: every number with its method, its conditions and its source.
Other names and standards
The same grade under other systems, as datasheets and standards print them. Each code was checked against the page it comes from.
| System | Codes |
|---|---|
| Trade name | IG-110 |
Notes
The method, full conditions and any caveat for the numbered rows above.
| # | Measurement | Method | Conditions | Caveat |
|---|---|---|---|---|
| 1 | Bulk density, pre-irradiation specimens | Measured by ORNL on pre-irradiation specimens and printed in the report table | form isostatically pressed IG-110, as receivedspecimens all specimen shapesreported as average plus or minus 1 sigma | Uncertainty: ± 0.017 (1σ) |
| 2 | Bulk density, ORNL 2022 Table 1 | Measured at ORNL and printed in Table 1 of the 2022 review | basis bulk density by mensuration, IG-110 columngrade column Isotropic | The 2018 ORNL report gives 1.77 and this 2022 table gives 1.761; both values are printed by ORNL and both are kept here. |
| 3 | Dynamic Young's modulus, MB specimens, axial | Dynamic Young's modulus measured by ORNL on pre-irradiation specimens | specimen shape MB, as printedorientation AX (axial, with gravity during pressing)temperature not printed in Table 2.2 | Uncertainty: ± 0.23 (1σ) |
| 4 | Dynamic Young's modulus, MB specimens, transverse | Dynamic Young's modulus measured by ORNL on pre-irradiation specimens | specimen shape MB, as printedorientation TR (transverse)temperature not printed in Table 2.2 | Uncertainty: ± 0.22 (1σ) |
| 5 | Compression strength, CRS specimens, axial | Compression test by ORNL on pre-irradiation specimens | specimen shape CRS, as printedorientation AX (axial)temperature not printed in Table 2.2 | Uncertainty: ± 3.3 (1σ) |
| 6 | Compression strength, CRS specimens, transverse | Compression test by ORNL on pre-irradiation specimens | specimen shape CRS, as printedorientation TR (transverse)temperature not printed in Table 2.2 | Uncertainty: ± 2.1 (1σ) |
| 7 | 4-point flexural strength, MB specimens, axial | 4-point flexural test by ORNL on a small subset of pre-irradiation specimens | test 4-point flexuralspecimen shape MB, as printedorientation AX (axial) | Uncertainty: ± 1.8 (1σ) |
| 8 | 4-point flexural strength, MB specimens, transverse | 4-point flexural test by ORNL on a small subset of pre-irradiation specimens | test 4-point flexuralspecimen shape MB, as printedorientation TR (transverse) | Uncertainty: ± 1.3 (1σ) |
| 9 | Mean coefficient of thermal expansion at 500 °C, MB axial | Mean CTE measured by ORNL; the source prints the unit as 10-6 K-1, and the number is unchanged in ppm/K | temperature mean CTE at 500 °C, as printedspecimen shape MB, as printedorientation AX (axial) | Uncertainty: ± 0.04 (1σ) |
| 10 | Mean coefficient of thermal expansion at 500 °C, MB transverse | Mean CTE measured by ORNL; the source prints the unit as 10-6 K-1, and the number is unchanged in ppm/K | temperature mean CTE at 500 °C, as printedspecimen shape MB, as printedorientation TR (transverse) | Uncertainty: ± 0.11 (1σ) |
| 11 | Isotropy ratio of thermal expansion | Ratio printed by ORNL in the same table as the CTE rows | basis ratio as printed in Table 2.2, pre-irradiation specimens | — |
| 12 | Thermal conductivity at 25 °C, TD4 specimens, axial | Thermal conductivity measured by ORNL on a few pre-irradiation specimens | temperature 25 °C, as printedspecimen shape TD4, as printedorientation AX (axial) | Uncertainty: ± 7.2 (1σ) |
| 13 | Thermal conductivity at 25 °C, TD4 specimens, transverse | Thermal conductivity measured by ORNL on a few pre-irradiation specimens | temperature 25 °C, as printedspecimen shape TD4, as printedorientation TR (transverse) | Uncertainty: ± 3.7 (1σ) |
| 14 | Thermal conductivity at 500 °C, TD4 specimens, axial | Thermal conductivity measured by ORNL on a few pre-irradiation specimens | temperature 500 °C, as printedspecimen shape TD4, as printedorientation AX (axial) | Uncertainty: ± 3.5 (1σ) |
| 15 | Thermal conductivity at 500 °C, TD4 specimens, transverse | Thermal conductivity measured by ORNL on a few pre-irradiation specimens | temperature 500 °C, as printedspecimen shape TD4, as printedorientation TR (transverse) | Uncertainty: ± 1.4 (1σ) |
| 16 | Average grain size | Printed by ORNL as an average value in the general properties table | basis average grain size, IG-110 column, as printed | — |
| 17 | Tensile strength, ORNL 2022 Table 1 | Printed by ORNL in the general properties table; the table does not name the test | basis IG-110 column of the general properties table; test method not printed | The test method is not printed. This is a different test from the 34 MPa flexural value in the 2018 report, so the two are not directly comparable. |
| 18 | Compressive strength, ORNL 2022 Table 1 | Printed by ORNL in the general properties table; the table does not name the test | basis IG-110 column of the general properties table; test method not printed | The test method is not printed. The 2018 report gives 77 MPa for axial compression specimens (Table 2.2), so the two sources are shown side by side. |
| 19 | Dynamic Young's modulus, ORNL 2022 Table 1 | — | basis IG-110 column of the general properties table | This 2022 value differs from the 9.1 GPa axial and 9.7 GPa transverse values in the 2018 report; both are kept. |
| 20 | Activation energy for air oxidation, Smith data set | Arrhenius fit of oxidation rate data for IG-110 in air, as tabulated by ORNL | atmosphere air (21% O2)temperature range 536 to 695 °Cflow rate 10 L/minspecimen cylinder, 2.54 D x 5.08 H cm | The same table gives 187 kJ/mol for the Fuller data set and 169 kJ/mol for the Chi data set, measured over other temperature ranges. |
| 21 | Activation energy for air oxidation, Fuller data set | Arrhenius fit of oxidation rate data for IG-110 in air, as tabulated by ORNL | atmosphere air (21% O2)temperature range 450 to 750 °Cflow rate 0.5 L/minspecimen cylinder, 0.84 D x 1.90 H cm | — |
| 22 | Activation energy for air oxidation, Chi data set | Arrhenius fit of oxidation rate data for IG-110 in air, as tabulated by ORNL | atmosphere air (21% O2)temperature range 603 to 808 °Cflow rate 10 L/minspecimen cylinder, 2.54 D x 2.54 H cm | — |
| 23 | Thermal conductivity after neutron irradiation, sample T11T15 | Post-irradiation thermal conductivity at 25 °C measured by ORNL on one specimen of the irradiation set | state after neutron irradiationspecimen TD3, TR orientationdesign temperature 300 °Cmeasured temperature 256 °Ctest temperature 25 °Cfluence printed in the source with an exponent, not reproduced here | One row of the appendix table; irradiated values in that table are far below the 129 W/m/K unirradiated axial value. |
| 24 | Volume change after neutron irradiation, sample T10T06 | Post-irradiation volume change (delta V over V0) measured by ORNL | state after neutron irradiationspecimen MB, TR orientationdesign temperature 300 °Cmeasured temperature 410 °Cfluence printed in the source with an exponent, not reproduced here | — |
Corrosion and compatibility
What happens when it meets other materials and environments.
| Environment | Concern | What happens |
|---|---|---|
| Air at high temperature (dry air, oxidation in the kinetic regime) | moderate | In air, IG-110 oxidizes, and the rate rises steeply with temperature.1 |
| Metal impurities in the graphite | moderate | Metal impurities can speed oxidation in an uncontrolled way.2 |
| # | Environment | Details | Test conditions |
|---|---|---|---|
| 1 | Air at high temperature (dry air, oxidation in the kinetic regime) | ORNL's 2022 review tabulates apparent activation energies for IG-110 oxidation in air of 195 kJ/mol (Smith data set) and 187 kJ/mol (Fuller data set). The review says the kinetic regime lies 'approximately between' the quoted range for specimens of the standard shape, provided oxidant supply is ample. | temperature 536 to 695 °C in the Smith data setatmosphere air |
| 2 | Metal impurities in the graphite | ORNL's review states that metal impurities that may act as oxidation catalysts may accelerate oxidation rates in an uncontrollable way. | basis general statement in the conclusions, not a measured IG-110 value |
Risks and side effects
Hazards to people, what happens when a cell overheats, and how the material is handled and stored.
For people
No safety data sheet for IG-110 itself was found. The nearest record is PubChem's Carbon entry.
- Dust
- Most company notifications in the Carbon record do not meet GHS hazard criteria. Where codes appear, they are eye irritation and respiratory irritation.
If it is heated in air
These results come from laboratory oxidation tests, not from incidents.
- Air oxidation
- Air oxidation of IG-110 has activation energies of 195 kJ/mol and 187 kJ/mol in two data sets. ORNL's review shows oxidation rates rising steeply with temperature.
In a reactor
Irradiation changes the material. ORNL's data show a large drop in conductivity and a measurable volume change.
- Thermal conductivity
- After irradiation, one specimen read 2.80 W/m/K at 25 °C, against 129 W/m/K before irradiation in the axial direction.
- Shape
- In another specimen the volume changed by -7.39% after irradiation.
Test details
The original wording and numbers from the sources, for readers who want them.
Failure risks
| Failure | Trigger and consequence |
|---|---|
| Oxidation of hot graphite in airhigh severity | Air at high temperature; the Smith data set covers 536 to 695 °COxidation rises steeply with temperature (activation energy 195 kJ/mol in the Smith data set). The review reports property changes after oxidation to 'nominally 2.5% and 7.5% weight loss' from older Japanese data, shown in figures only. |
| Thermal conductivity loss under neutron irradiationhigh severity | Neutron irradiation at a 300 °C design temperatureThermal conductivity at 25 °C falls to 2.80 W/m/K in the sampled specimen, against 129 W/m/K axially before irradiation. |
| Dimensional change under neutron irradiationmoderate severity | Neutron irradiation at a 300 °C design temperature and 410 °C measured temperatureVolume changes by -7.39% in sample T10T06 (MB, TR). ORNL reports that length change differs between the two orientations, which it calls unexpected for near-isotropic graphite. |
Side effects on surrounding parts
| Affects | Effect |
|---|---|
| Core graphite in a reactor, where heat must still leave the graphite | Irradiation changes the dimensions and the thermal properties of the same graphite, so a part can change shape and lose conduction at the same time (ORNL reports both). |
Handling and storage
- PubChem's Carbon record gives precautionary statement codes for handling, but the wording of those codes is not printed in the record fetched in this run.
- ORNL measured the oxidation of IG-110 in air at high temperature, so hot graphite should be kept away from air where the process allows.
Mitigations
- ORNL states it is "imperative" to examine property changes in both distinct directions after irradiation, because length change differed between them.
Supply and geography
How common the raw materials are and where they come from.
Graphite, natural (USGS covers natural graphite; IG-110 is a synthetic grade)
World resources exceed 800 million tons of recoverable graphite outside the United States (USGS, World Resources).
- Top producers (2025)
- China 82%, Madagascar 4.4%, Tanzania 4.2%
- Critical mineral lists
- EU: listed
- Recycling
- USGS: 'The abundance of graphite in the world market inhibits increased recycling efforts.'
- Substitutes
- USGS: synthetic graphite powder, scrap from machined shapes and calcined petroleum coke compete for iron and steel uses; synthetic graphite powder and secondary synthetic graphite from machined shapes compete for battery uses.
Documents
Datasheets, safety data sheets, papers and standards you can open.
Full record
The complete spore, as stored. Free to reuse under CC-BY-4.0. Images keep the licence shown with each one.
Show the full YAML
spore: profile
id: ig-110-isotropic-graphite
spore_version: 0.2
family: carbon-materials
name: IG-110 isotropic graphite
abbreviation: IG-110
role: isostatically pressed nuclear graphite grade (Toyo Tanso), studied by ORNL for a high-temperature gas-cooled reactor
category: carbon
type: graphite
summary: |
IG-110 is a fine-grained, isostatically pressed graphite made by Toyo Tanso and qualified by Oak Ridge National Laboratory (ORNL) as a candidate material for a high-temperature gas-cooled reactor. ORNL measured a bulk density of 1.77 g/cm3 before irradiation, per its 2018 summary report. Neutron irradiation sharply lowered thermal conductivity: one specimen irradiated at a measured 256 degC read 2.80 W/m/K at 25 degC, against 129 W/m/K before irradiation in the axial direction.
best_for: Reference nuclear graphite where ORNL baseline and irradiation data for the grade matter, such as reactor-core qualification studies
weakest_at: 'Irradiation and air oxidation: thermal conductivity falls sharply after neutron irradiation, and the graphite oxidizes in air at high temperature'
identity:
formula: C (carbon; synthetic graphite made from petroleum-based carbon materials)
designations:
- system: Trade name
code: IG-110
source: ornl-tm2018-1040
where: Section 2.1 (Grade IG-110, Toyo Tanso Co., Ltd.)
source: ornl-tm2022-1839
where: Table 1 (manufacturer Toyo Tanso, LTD; coke type Petroleum; forming method Isostatically pressed)
tags:
environments: []
stresses:
- extreme-heat
applications:
- structures
- electronics-and-chips
properties:
- benchmark: density
label: Bulk density, pre-irradiation specimens
value: 1.77
unit: g/cm3
scope: material
conditions:
form: isostatically pressed IG-110, as received
specimens: all specimen shapes
reported_as: average plus or minus 1 sigma
method: Measured by ORNL on pre-irradiation specimens and printed in the report table
uncertainty: ± 0.017 (1σ)
status: ground
source: ornl-tm2018-1040
where: Table 2.2 (page 3), Density (g/cm3), all specimens
- benchmark: density
label: Bulk density, ORNL 2022 Table 1
value: 1.761
unit: g/cm3
scope: material
conditions:
basis: bulk density by mensuration, IG-110 column
grade_column: Isotropic
method: Measured at ORNL and printed in Table 1 of the 2022 review
status: ground
note: The 2018 ORNL report gives 1.77 and this 2022 table gives 1.761; both values are printed by ORNL and both are kept here.
source: ornl-tm2022-1839
where: Table 1, row Bulk density (mensuration)
- benchmark: elastic_modulus
label: Dynamic Young's modulus, MB specimens, axial
value: 9.1
unit: GPa
scope: material
conditions:
specimen_shape: MB, as printed
orientation: AX (axial, with gravity during pressing)
temperature: not printed in Table 2.2
method: Dynamic Young's modulus measured by ORNL on pre-irradiation specimens
uncertainty: ± 0.23 (1σ)
status: ground
source: ornl-tm2018-1040
where: Table 2.2 (page 3), Dynamic Young's Modulus (GPa), MB, AX
- benchmark: elastic_modulus
label: Dynamic Young's modulus, MB specimens, transverse
value: 9.7
unit: GPa
scope: material
conditions:
specimen_shape: MB, as printed
orientation: TR (transverse)
temperature: not printed in Table 2.2
method: Dynamic Young's modulus measured by ORNL on pre-irradiation specimens
uncertainty: ± 0.22 (1σ)
status: ground
source: ornl-tm2018-1040
where: Table 2.2 (page 3), Dynamic Young's Modulus (GPa), MB, TR
- benchmark: compressive_strength
label: Compression strength, CRS specimens, axial
value: 77
unit: MPa
scope: material
conditions:
specimen_shape: CRS, as printed
orientation: AX (axial)
temperature: not printed in Table 2.2
method: Compression test by ORNL on pre-irradiation specimens
uncertainty: ± 3.3 (1σ)
status: ground
source: ornl-tm2018-1040
where: Table 2.2 (page 3), Compression Strength (MPa), CRS, AX
- benchmark: compressive_strength
label: Compression strength, CRS specimens, transverse
value: 77
unit: MPa
scope: material
conditions:
specimen_shape: CRS, as printed
orientation: TR (transverse)
temperature: not printed in Table 2.2
method: Compression test by ORNL on pre-irradiation specimens
uncertainty: ± 2.1 (1σ)
status: ground
source: ornl-tm2018-1040
where: Table 2.2 (page 3), Compression Strength (MPa), CRS, TR
- benchmark: flexural_strength
label: 4-point flexural strength, MB specimens, axial
value: 34
unit: MPa
scope: material
conditions:
test: 4-point flexural
specimen_shape: MB, as printed
orientation: AX (axial)
method: 4-point flexural test by ORNL on a small subset of pre-irradiation specimens
uncertainty: ± 1.8 (1σ)
status: ground
source: ornl-tm2018-1040
where: Table 2.2 (page 3), 4-point Flexural Strength (MPa), MB, AX
- benchmark: flexural_strength
label: 4-point flexural strength, MB specimens, transverse
value: 36
unit: MPa
scope: material
conditions:
test: 4-point flexural
specimen_shape: MB, as printed
orientation: TR (transverse)
method: 4-point flexural test by ORNL on a small subset of pre-irradiation specimens
uncertainty: ± 1.3 (1σ)
status: ground
source: ornl-tm2018-1040
where: Table 2.2 (page 3), 4-point Flexural Strength (MPa), MB, TR
- benchmark: cte
label: Mean coefficient of thermal expansion at 500 °C, MB axial
value: 4.5
unit: ppm/K
scope: material
conditions:
temperature: mean CTE at 500 °C, as printed
specimen_shape: MB, as printed
orientation: AX (axial)
method: Mean CTE measured by ORNL; the source prints the unit as 10-6 K-1, and the number is unchanged in ppm/K
uncertainty: ± 0.04 (1σ)
status: ground
source: ornl-tm2018-1040
where: Table 2.2 (page 3), Mean CTE at 500°C (10-6 K-1), MB, AX
- benchmark: cte
label: Mean coefficient of thermal expansion at 500 °C, MB transverse
value: 4.2
unit: ppm/K
scope: material
conditions:
temperature: mean CTE at 500 °C, as printed
specimen_shape: MB, as printed
orientation: TR (transverse)
method: Mean CTE measured by ORNL; the source prints the unit as 10-6 K-1, and the number is unchanged in ppm/K
uncertainty: ± 0.11 (1σ)
status: ground
source: ornl-tm2018-1040
where: Table 2.2 (page 3), Mean CTE at 500°C (10-6 K-1), MB, TR
- benchmark: isotropy_ratio
label: Isotropy ratio of thermal expansion
value: 1.057
unit: '-'
scope: material
conditions:
basis: ratio as printed in Table 2.2, pre-irradiation specimens
method: Ratio printed by ORNL in the same table as the CTE rows
status: ground
source: ornl-tm2018-1040
where: Table 2.2 (page 3), Isotropy Ratio
- benchmark: thermal_conductivity
label: Thermal conductivity at 25 °C, TD4 specimens, axial
value: 129
unit: W/m/K
scope: material
conditions:
temperature: 25 °C, as printed
specimen_shape: TD4, as printed
orientation: AX (axial)
method: Thermal conductivity measured by ORNL on a few pre-irradiation specimens
uncertainty: ± 7.2 (1σ)
status: ground
source: ornl-tm2018-1040
where: Table 2.2 (page 3), Thermal Conductivity at 25°C (W/m/K), TD4, AX
- benchmark: thermal_conductivity
label: Thermal conductivity at 25 °C, TD4 specimens, transverse
value: 130
unit: W/m/K
scope: material
conditions:
temperature: 25 °C, as printed
specimen_shape: TD4, as printed
orientation: TR (transverse)
method: Thermal conductivity measured by ORNL on a few pre-irradiation specimens
uncertainty: ± 3.7 (1σ)
status: ground
source: ornl-tm2018-1040
where: Table 2.2 (page 3), Thermal Conductivity at 25°C (W/m/K), TD4, TR
- benchmark: thermal_conductivity
label: Thermal conductivity at 500 °C, TD4 specimens, axial
value: 73
unit: W/m/K
scope: material
conditions:
temperature: 500 °C, as printed
specimen_shape: TD4, as printed
orientation: AX (axial)
method: Thermal conductivity measured by ORNL on a few pre-irradiation specimens
uncertainty: ± 3.5 (1σ)
status: ground
source: ornl-tm2018-1040
where: Table 2.2 (page 3), Thermal Conductivity at 500°C (W/m/K), TD4, AX
- benchmark: thermal_conductivity
label: Thermal conductivity at 500 °C, TD4 specimens, transverse
value: 77
unit: W/m/K
scope: material
conditions:
temperature: 500 °C, as printed
specimen_shape: TD4, as printed
orientation: TR (transverse)
method: Thermal conductivity measured by ORNL on a few pre-irradiation specimens
uncertainty: ± 1.4 (1σ)
status: ground
source: ornl-tm2018-1040
where: Table 2.2 (page 3), Thermal Conductivity at 500°C (W/m/K), TD4, TR
- benchmark: grain_size
label: Average grain size
value: 20
unit: µm
scope: material
conditions:
basis: average grain size, IG-110 column, as printed
method: Printed by ORNL as an average value in the general properties table
status: ground
source: ornl-tm2022-1839
where: Table 1, row Grain size (µm), IG-110 column
- benchmark: ash_content
label: Ash content
value: 10
bound: upper
unit: ppm
scope: material
conditions:
basis: printed as less than 10 ppm
method: Printed by ORNL in the general properties table
status: ground
source: ornl-tm2022-1839
where: Table 1, row Ash content (ppm), IG-110 column
- benchmark: ultimate_tensile_strength
label: Tensile strength, ORNL 2022 Table 1
value: 14.9
unit: MPa
scope: material
conditions:
basis: IG-110 column of the general properties table; test method not printed
method: Printed by ORNL in the general properties table; the table does not name the test
status: ground
note: The test method is not printed. This is a different test from the 34 MPa flexural value in the 2018 report, so the two are not directly comparable.
source: ornl-tm2022-1839
where: Table 1, row Tensile strength (MPa), IG-110 column
- benchmark: compressive_strength
label: Compressive strength, ORNL 2022 Table 1
value: 73.44
unit: MPa
scope: material
conditions:
basis: IG-110 column of the general properties table; test method not printed
method: Printed by ORNL in the general properties table; the table does not name the test
status: ground
note: The test method is not printed. The 2018 report gives 77 MPa for axial compression specimens (Table 2.2), so the two sources are shown side by side.
source: ornl-tm2022-1839
where: Table 1, row Compressive strength (MPa), IG-110 column
- benchmark: elastic_modulus
label: Dynamic Young's modulus, ORNL 2022 Table 1
value: 8.767
unit: GPa
scope: material
conditions:
basis: IG-110 column of the general properties table
method: Printed by ORNL in the general properties table
status: ground
note: This 2022 value differs from the 9.1 GPa axial and 9.7 GPa transverse values in the 2018 report; both are kept.
source: ornl-tm2022-1839
where: Table 1, row Dynamic young's modulus (GPa), IG-110 column
- benchmark: poissons_ratio
label: Poisson's ratio
value: 0.157
unit: '-'
scope: material
conditions:
basis: IG-110 column of the general properties table
method: Printed by ORNL in the general properties table
status: ground
source: ornl-tm2022-1839
where: Table 1, row Poisson ratio, IG-110 column
- benchmark: oxidation_activation_energy
label: Activation energy for air oxidation, Smith data set
value: 195
unit: kJ/mol
scope: material
conditions:
atmosphere: air (21% O2)
temperature_range: 536 to 695 °C
flow_rate: 10 L/min
specimen: cylinder, 2.54 D x 5.08 H cm
method: Arrhenius fit of oxidation rate data for IG-110 in air, as tabulated by ORNL
status: ground
note: The same table gives 187 kJ/mol for the Fuller data set and 169 kJ/mol for the Chi data set, measured over other temperature ranges.
source: ornl-tm2022-1839
where: Table 3 (Selected kinetic parameters oxidation of IG-110 by air), Smith row
- benchmark: oxidation_activation_energy
label: Activation energy for air oxidation, Fuller data set
value: 187
unit: kJ/mol
scope: material
conditions:
atmosphere: air (21% O2)
temperature_range: 450 to 750 °C
flow_rate: 0.5 L/min
specimen: cylinder, 0.84 D x 1.90 H cm
method: Arrhenius fit of oxidation rate data for IG-110 in air, as tabulated by ORNL
status: ground
source: ornl-tm2022-1839
where: Table 3 (Selected kinetic parameters oxidation of IG-110 by air), Fuller row
- benchmark: oxidation_activation_energy
label: Activation energy for air oxidation, Chi data set
value: 169
unit: kJ/mol
scope: material
conditions:
atmosphere: air (21% O2)
temperature_range: 603 to 808 °C
flow_rate: 10 L/min
specimen: cylinder, 2.54 D x 2.54 H cm
method: Arrhenius fit of oxidation rate data for IG-110 in air, as tabulated by ORNL
status: ground
source: ornl-tm2022-1839
where: Table 3 (Selected kinetic parameters oxidation of IG-110 by air), Chi row
- benchmark: thermal_conductivity
label: Thermal conductivity after neutron irradiation, sample T11T15
value: 2.8
unit: W/m/K
scope: material
conditions:
state: after neutron irradiation
specimen: TD3, TR orientation
design_temperature: 300 °C
measured_temperature: 256 °C
test_temperature: 25 °C
fluence: printed in the source with an exponent, not reproduced here
method: Post-irradiation thermal conductivity at 25 °C measured by ORNL on one specimen of the irradiation set
status: ground
note: One row of the appendix table; irradiated values in that table are far below the 129 W/m/K unirradiated axial value.
source: ornl-tm2018-1040
where: Appendix B.5.1 (Room Temperature), row T11T15
- benchmark: volume_change
label: Volume change after neutron irradiation, sample T10T06
value: -7.39
unit: '%'
scope: material
conditions:
state: after neutron irradiation
specimen: MB, TR orientation
design_temperature: 300 °C
measured_temperature: 410 °C
fluence: printed in the source with an exponent, not reproduced here
method: Post-irradiation volume change (delta V over V0) measured by ORNL
status: ground
source: ornl-tm2018-1040
where: Appendix B.1 (Post-irradiation dimension and Young's modulus), row T10T06
corrosion:
- environment: Air at high temperature (dry air, oxidation in the kinetic regime)
headline: In air, IG-110 oxidizes, and the rate rises steeply with temperature.
effect: ORNL's 2022 review tabulates apparent activation energies for IG-110 oxidation in air of 195 kJ/mol (Smith data set) and 187 kJ/mol (Fuller data set). The review says the kinetic regime lies 'approximately between' the quoted range for specimens of the standard shape, provided oxidant supply is ample.
rating: moderate
conditions:
temperature: 536 to 695 °C in the Smith data set
atmosphere: air
source: ornl-tm2022-1839
where: Table 3 and Section 4.3.5 (Conclusions on Acute Oxidation Tests)
- environment: Metal impurities in the graphite
headline: Metal impurities can speed oxidation in an uncontrolled way.
effect: ORNL's review states that metal impurities that may act as oxidation catalysts may accelerate oxidation rates in an uncontrollable way.
rating: moderate
conditions:
basis: general statement in the conclusions, not a measured IG-110 value
source: ornl-tm2022-1839
where: Section 4.3.5 (Conclusions on Acute Oxidation Tests), last bullet
risks:
hazards:
- text: 'PubChem''s Carbon record says: ''This chemical does not meet GHS hazard criteria for 40.2% (1095 of 2727) of reports.'' No graphite-specific safety data sheet for IG-110 was found in this run.'
ghs: []
source: pubchem-carbon
where: GHS Classification section of the Carbon record (CID 5462310)
- text: The Carbon record lists eye-irritation and respiratory-irritation codes for some company notifications only. It is an element entry, not a record for IG-110.
ghs:
- H319
- H335
source: pubchem-carbon
where: GHS Classification section, Hazard Statements list
failure_risks:
- mode: Oxidation of hot graphite in air
trigger: Air at high temperature; the Smith data set covers 536 to 695 °C
consequence: Oxidation rises steeply with temperature (activation energy 195 kJ/mol in the Smith data set). The review reports property changes after oxidation to 'nominally 2.5% and 7.5% weight loss' from older Japanese data, shown in figures only.
severity: high
source: ornl-tm2022-1839
where: Table 3 and Section 5.3 (Degradation of oxidized graphite IG-110 properties)
- mode: Thermal conductivity loss under neutron irradiation
trigger: Neutron irradiation at a 300 °C design temperature
consequence: Thermal conductivity at 25 °C falls to 2.80 W/m/K in the sampled specimen, against 129 W/m/K axially before irradiation.
severity: high
source: ornl-tm2018-1040
where: Appendix B.5.1 and Table 2.2
- mode: Dimensional change under neutron irradiation
trigger: Neutron irradiation at a 300 °C design temperature and 410 °C measured temperature
consequence: Volume changes by -7.39% in sample T10T06 (MB, TR). ORNL reports that length change differs between the two orientations, which it calls unexpected for near-isotropic graphite.
severity: moderate
source: ornl-tm2018-1040
where: Appendix B.1 and Section 4 conclusions
side_effects:
- text: Irradiation changes the dimensions and the thermal properties of the same graphite, so a part can change shape and lose conduction at the same time (ORNL reports both).
affects: Core graphite in a reactor, where heat must still leave the graphite
source: ornl-tm2018-1040
where: Section 4 conclusions and Appendix B
handling:
- text: PubChem's Carbon record gives precautionary statement codes for handling, but the wording of those codes is not printed in the record fetched in this run.
source: pubchem-carbon
where: Safety and Hazards, Precautionary Statements
- text: ORNL measured the oxidation of IG-110 in air at high temperature, so hot graphite should be kept away from air where the process allows.
source: ornl-tm2022-1839
where: Section 4.3.2 (Graphite IG-110)
mitigations:
- text: ORNL states it is "imperative" to examine property changes in both distinct directions after irradiation, because length change differed between them.
source: ornl-tm2018-1040
where: Section 4 conclusions
uses:
- application: structures
device: Core graphite structures in a high-temperature gas-cooled reactor (candidate material, not a deployed use)
example: ORNL and Toyo Tanso ran a joint program to qualify IG-110 as a candidate material for use in the Generation-IV high temperature gas-cooled nuclear reactor.
source: ornl-tm2017-705
where: Section 1 (Introduction)
- application: electronics-and-chips
device: Semiconductor manufacturing parts made from isotropic graphite (the industry is named; IG-110 is not named)
example: Toyo Tanso names the semiconductor industry, where innovation is rapidly advancing, as a user of its isotropic graphite.
source: toyo-tanso-special
where: Industries section of the special graphite page
supply:
- subject: Graphite, natural (USGS covers natural graphite; IG-110 is a synthetic grade)
abundance: World resources exceed 800 million tons of recoverable graphite outside the United States (USGS, World Resources).
producers:
- country: China
share_percent: 82
year: 2025
- country: Madagascar
share_percent: 4.4
year: 2025
- country: Tanzania
share_percent: 4.2
year: 2025
critical_lists:
- list: EU critical raw materials, Fifth list 2023 (Natural Graphite is listed; the Commission page does not mark it strategic)
listed: true
recycling: 'USGS: ''The abundance of graphite in the world market inhibits increased recycling efforts.'''
substitutes:
- 'USGS: synthetic graphite powder, scrap from machined shapes and calcined petroleum coke compete for iron and steel uses; synthetic graphite powder and secondary synthetic graphite from machined shapes compete for battery uses.'
source: usgs-mcs2026-graphite
where: World Mine Production and Reserves table, 2025e (world total 1,800,000 t, rounded); China share from the text (estimated 82% of total world production); Madagascar and Tanzania shares calculated by Space Mushroom from 80,000 t and 75,000 t against the 1,800,000 t total. EU list status from the European Commission page (source key ec-crm).
media: []
documents:
- title: 'ORNL/TM-2018/1040: Summary Report on Effects of Irradiation on Material IG-110 (prepared for Toyo Tanso Co., Ltd.)'
type: report
url: https://info.ornl.gov/sites/publications/Files/Pub118793.pdf
year: 2018
- title: 'ORNL/TM-2017/705: Report on Effects of Irradiation on Material IG-110'
type: report
url: https://info.ornl.gov/sites/publications/Files/Pub104952.pdf
year: 2017
- title: 'ORNL/TM-2022/1839: Oxidation Behavior and Property Degradation of Nuclear Graphites'
type: report
url: https://info.ornl.gov/sites/publications/Files/Pub172937.pdf
year: 2022
- title: 'PubChem compound record: Carbon (CID 5462310), GHS classification'
type: database
url: https://pubchem.ncbi.nlm.nih.gov/compound/5462310
year: 2026
- title: 'USGS Mineral Commodity Summaries 2026: Graphite (Natural)'
type: report
url: https://pubs.usgs.gov/periodicals/mcs2026/mcs2026-graphite.pdf
year: 2026
- title: Toyo Tanso special graphite property data page (lists IG-11, not IG-110)
type: datasheet
url: https://www.toyotanso.com/Products/Special_graphite/data.html
gaps:
- No IG-110 safety data sheet was found. The hazard entries use PubChem's Carbon record (CID 5462310), an element entry, not a graphite-specific record.
- The Toyo Tanso property data page lists IG-11 but not IG-110, so no manufacturer datasheet value for IG-110 is used.
- Irradiation values are recorded for one thermal conductivity row and one volume change row only. Fluence is printed with an exponent in the source and is left out. Irradiated strength, modulus, CTE and creep values are not recorded.
- Oxidation rate constants (pre-exponential factors) are printed with exponents, so they are left out. Oxidized strength and fracture-toughness changes (ORNL 2022 Section 5.3) are shown in figures only.
- 'Density differs between ORNL sources: 1.77 g/cm3 (2018 report) and 1.761 g/cm3 (2022 review). Both are kept; the difference is not resolved.'
- The 2022 review's tensile and compressive values do not name the test method. The porosity column layout in the extracted text is unclear, so no porosity value is recorded.
- Thermal conductivity and CTE at temperatures other than 25 and 500 °C were not found for IG-110 in these sources.
- Supply data cover natural graphite only (USGS). No production-country data for synthetic isostatically pressed graphite such as IG-110 was found.
- USGS 2025 critical minerals list status for graphite was not verified in this run. The EU list status is recorded.
- Carbon atomic weight and atom counts were not read; the recipe gives components, not a formula ratio.
- No space flight, vacuum or space-radiation data were found. The irradiation data are reactor tests (HFIR at ORNL).
- 'Non-canonical property names used: grain_size, ash_content, compressive_strength, volume_change, isotropy_ratio, oxidation_activation_energy.'
license: CC-BY-4.0
updated: '2026-11-02'
review:
status: draft
method: assistant
checked_values: 26
unreachable: 0
caveats: 2
note: 'Values re-read by an AI assistant on 2026-11-02 from the ORNL PDFs (text extracted with pdftotext) and the USGS graphite summary. Two values carry caveats: the 2022 density and tensile test method.'
story:
recipe:
line: IG-110 is a synthetic graphite made from petroleum-based carbon materials and formed by isostatic pressing. ORNL describes nuclear graphite as a composite of filler, binder and pores, and says the vendor's process details are proprietary.
parts:
- name: Carbon filler
symbol: C
role: Carbon particles from a petroleum-based coke that form most of the graphite skeleton
source: ornl-tm2022-1839
where: Section 3 (Structure and properties) and Table 1, coke type Petroleum
- name: Binder carbon
role: Carbon that binds the filler together after forming, baking and graphitization
source: ornl-tm2022-1839
where: Section 3 (filler, binder and pores; manufacturing sequence)
- name: Pores
role: Open and closed voids that set the density and strength of the finished block
source: ornl-tm2022-1839
where: Section 3 and Table 2 (pore volumes)
why: IG-110 is an isotropic nuclear graphite made by Toyo Tanso. Isotropic means its properties are nearly the same in every direction. ORNL and Toyo Tanso ran a joint program to qualify it for a Generation-IV high temperature gas-cooled reactor. The program measured its baseline properties and how neutron irradiation changes them, and the results are published in ORNL reports.
uses:
- where: Reactor core candidate
line: ORNL and Toyo Tanso qualified IG-110 as a candidate material for a Generation-IV high temperature gas-cooled reactor. The sources we hold describe this as a qualification role, not a deployed use.
- where: Semiconductor industry
line: Toyo Tanso names the semiconductor industry as a user of its isotropic graphite. Its page does not name IG-110 in that list, so this is an industry-level claim.
can_do:
- label: Density
benchmark: density
line: ORNL measured a bulk density of 1.77 g/cm3 before irradiation, so one cubic centimetre of the graphite weighs about 1.77 grams.
- label: Grain size
benchmark: grain_size
line: The average grain size is 20 µm, printed in ORNL's 2022 review. This is the finest of the three nuclear graphites that review compares.
- label: Strength
benchmark: flexural_strength
line: Flexural strength is 34 MPa in the axial direction and 36 MPa in the transverse direction, before irradiation, in ORNL's 2018 report.
- label: Heat conduction
benchmark: thermal_conductivity
line: Thermal conductivity at 25 °C is 129 W/m/K in the axial direction before irradiation. After irradiation, one specimen read 2.80 W/m/K.
- label: Oxidation in air
benchmark: oxidation_activation_energy
line: Air oxidation has an activation energy of 195 kJ/mol in one data set and 187 kJ/mol in another, both printed in ORNL's 2022 review.
compare: Among the three nuclear graphites that ORNL compares in its 2022 review, IG-110 has by far the finest average grain. PCEA is extruded and NBG-18 is vibrationally molded, while IG-110 is isostatically pressed. The forming method and the fine grain are the two features that separate IG-110 from the other two grades in that review.
compare_rows:
- label: Bulk density
benchmark: density
- label: Thermal conductivity at 25 °C
benchmark: thermal_conductivity
- label: Air oxidation activation energy
benchmark: oxidation_activation_energy
handling:
- Keep hot graphite away from air where the process allows. ORNL measured oxidation of IG-110 in air at high temperature.
- The hazard data are thin. The nearest record, PubChem's Carbon entry, lists eye and respiratory irritation codes for some company notifications, so control dust.
good_for:
- Reference data. ORNL measured baseline values for IG-110 in two reports and one 2022 review.
- Reactor-core qualification work, where irradiation data for this grade already exist.
- 'Parts that need similar strength in both directions: the flexural strength is 34 MPa axially and 36 MPa transversely.'
watch_out:
- Thermal conductivity falls sharply after irradiation. One specimen dropped from 129 W/m/K to 2.80 W/m/K.
- Hot IG-110 oxidizes in air. The 2022 review reports activation energies of 195 kJ/mol and 187 kJ/mol.
- 'Density differs between ORNL sources: 1.77 g/cm3 in the 2018 report and 1.761 g/cm3 in the 2022 review.'
verdict: IG-110 is a well-documented nuclear graphite with ORNL baseline and irradiation data. Its weak points are irradiation-driven conductivity loss and oxidation in air at high temperature.
risk_groups:
- title: For people
level: 1
verdict: No IG-110 hazard data found; nearest is carbon
lead: No safety data sheet for IG-110 itself was found. The nearest record is PubChem's Carbon entry.
points:
- label: Dust
line: Most company notifications in the Carbon record do not meet GHS hazard criteria. Where codes appear, they are eye irritation and respiratory irritation.
- title: If it is heated in air
level: 2
verdict: Oxidizes in air when hot
lead: These results come from laboratory oxidation tests, not from incidents.
points:
- label: Air oxidation
line: Air oxidation of IG-110 has activation energies of 195 kJ/mol and 187 kJ/mol in two data sets. ORNL's review shows oxidation rates rising steeply with temperature.
- title: In a reactor
level: 3
verdict: Irradiation cuts thermal conductivity sharply
lead: Irradiation changes the material. ORNL's data show a large drop in conductivity and a measurable volume change.
points:
- label: Thermal conductivity
line: After irradiation, one specimen read 2.80 W/m/K at 25 °C, against 129 W/m/K before irradiation in the axial direction.
- label: Shape
line: In another specimen the volume changed by -7.39% after irradiation.
sources:
ornl-tm2018-1040:
title: Summary Report on Effects of Irradiation on Material IG-110 (ORNL/TM-2018/1040)
id: ORNL/TM-2018/1040
url: https://info.ornl.gov/sites/publications/Files/Pub118793.pdf
year: 2018
kind: report
license: Approved for public release; distribution is unlimited (ORNL)
ornl-tm2017-705:
title: Report on Effects of Irradiation on Material IG-110 (ORNL/TM-2017/705)
id: ORNL/TM-2017/705
url: https://info.ornl.gov/sites/publications/Files/Pub104952.pdf
year: 2017
kind: report
license: Approved for public release; distribution is unlimited (ORNL)
ornl-tm2022-1839:
title: Oxidation Behavior and Property Degradation of Nuclear Graphites (ORNL/TM-2022/1839)
id: ORNL/TM-2022/1839 (Contescu and Paul, March 2022)
url: https://info.ornl.gov/sites/publications/Files/Pub172937.pdf
year: 2022
kind: report
license: Approved for public release; distribution is unlimited (ORNL)
toyo-tanso-special:
title: Toyo Tanso special graphite (isotropic graphite applications)
url: https://www.toyotanso.com/Products/Special_graphite/
kind: web
license: Manufacturer web page, linked not reproduced
toyo-tanso-data:
title: Toyo Tanso special graphite property data (lists IG-11, not IG-110)
url: https://www.toyotanso.com/Products/Special_graphite/data.html
kind: datasheet
license: Manufacturer web page, linked not reproduced
usgs-mcs2026-graphite:
title: 'Mineral Commodity Summaries 2026: Graphite (Natural)'
id: USGS MCS 2026, February 2026
url: https://pubs.usgs.gov/periodicals/mcs2026/mcs2026-graphite.pdf
year: 2026
kind: report
license: public domain (USGS)
pubchem-carbon:
title: 'PubChem compound record: Carbon (CID 5462310), GHS classification'
id: CID 5462310
url: https://pubchem.ncbi.nlm.nih.gov/compound/5462310
year: 2026
kind: database
license: public domain (NCBI)
ec-crm:
title: Critical raw materials (European Commission, Fifth list 2023 of critical raw materials for the EU)
url: https://single-market-economy.ec.europa.eu/sectors/raw-materials/areas-specific-interest/critical-raw-materials_en
year: 2023
kind: web
license: European Commission web page
References
Every number above carries a reference number. Click one to see the source and where in it the value comes from.
| # | Source | Type | Year | Used for |
|---|---|---|---|---|
| Summary Report on Effects of Irradiation on Material IG-110 (ORNL/TM-2018/1040) | report | 2018 | 20 values | |
| Report on Effects of Irradiation on Material IG-110 (ORNL/TM-2017/705) | report | 2017 | 1 value | |
| Oxidation Behavior and Property Degradation of Nuclear Graphites (ORNL/TM-2022/1839) | report | 2022 | 15 values | |
| Toyo Tanso special graphite (isotropic graphite applications) | web | 1 value | ||
| Toyo Tanso special graphite property data (lists IG-11, not IG-110) | datasheet | 0 values | ||
| Mineral Commodity Summaries 2026: Graphite (Natural) | report | 2026 | 1 value | |
| PubChem compound record: Carbon (CID 5462310), GHS classification | database | 2026 | 3 values | |
| Critical raw materials (European Commission, Fifth list 2023 of critical raw materials for the EU) | web | 2023 | 0 values |
Updated