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Policy, Economics & Reactor Types · C-PE-001

Reactor Coolant Selection and Reactor-Type Comparison — How Water, Gas, Liquid Metal and Molten Salt Set Pressure and Temperature

Why water reactors need 15.5 MPa while sodium, lead and salt run hot near atmospheric pressure: heat capacity, conductivity, pumping power, activation and chemistry compared.

Definition

A reactor coolant is the fluid that removes the heat generated in the core and carries it toward the steam generators and turbine. A good coolant stores and conducts plenty of heat (high ρcₚ and k), flows with little pumping power, does not boil at low pressure, absorbs few neutrons and is little activated, is chemically compatible with structural materials, and is cheap.

The choice of coolant largely fixes a reactor type's pressure, temperature and neutron spectrum.

Principle and mechanism

Seven requirements

CategoryRequirementWhy it matters
ThermalHigh volumetric heat capacity ρcₚ, high thermal conductivity kHeat carried with less flow; smaller cladding-to-coolant temperature difference
HydraulicLow viscosity, low pumping powerSmaller house load and pumps
Phase changeHigh boiling point, low melting pointLow-pressure operation, no freezing
NuclearLow neutron absorption σaNeutron economy in thermal reactors; fast reactors also need little moderation
ActivationLow induced activity, short half-livesDose and maintenance access
ChemicalCompatible with fuel, cladding and structures; little reaction with water and air; stable under radiolysisPrevents corrosion, fire and hydrogen
Economy and safetyCheap and plentiful, easy to purify, favorable reactivity feedbackOperating cost, inherent safety

No coolant meets every requirement, so what was sacrificed and which design features compensate for it define the character of each reactor type.

The requirements in numbers

Comparison of seven coolants: volumetric heat capacity bars (FLiBe 4.68, water 4.02, Pb 1.55, LBE 1.48, Na 1.07, CO2 0.032, He 0.023 MJ per cubic metre kelvin), thermal conductivity (Na about 66, Pb about 17, water 0.55 W/m K), and relative pumping power on a log scale with water as 1 (FLiBe 3.5, Pb 235, LBE 241, Na 57, CO2 about 46,000, He about 29,000), with typical-temperature-rise values of 0.85 for Na, 6.5 for Pb, 15 for He and 63 for CO2, plus the formula pumping power proportional to mu^0.2 over rho squared cp^2.8
The cost of carrying heat. Relative pumping power for the same thermal power and flow geometry (H₂O = 1), with the effect of a typical temperature rise; not an actual pump or blower power ratio.

To carry thermal power Q with a temperature rise ΔT requires a mass flow ṁ = Q/(cₚΔT). Assuming a turbulent friction factor f ∝ Re−0.2, the same flow geometry and constant properties, the pumping power is Ẇ ∝ μ0.2/(ρ²cₚ2.8) (the same form as El-Wakil's coolant figure of merit). It is a relative hydraulic power under identical conditions, not an actual pump or blower power ratio.

Coolant (condition)ρcₚ [MJ/m³·K]Pumping-power index (H₂O = 1)k [W/m·K]Melting / boiling point at 1 atm [°C]
H₂O (15.5 MPa, 307 °C)4.0210.550 / 100
FLiBe (650 °C)4.683.5about 1.1459 / about 1,430
Na (450 °C)1.0757about 6698 / 883
Pb (450 °C)1.55235about 17327 / 1,749
CO₂ (4 MPa, 500 °C)0.032about 46,000about 0.05—
He (7 MPa, 500 °C)0.023about 29,000about 0.3—

Properties were calculated from IAPWS-IF97 (water), Fink & Leibowitz (Na), the OECD/NEA handbook (Pb), Romatoski & Hu (FLiBe) and the ideal-gas law (gases).

Water and molten salt are strong at storing heat (ρcₚ); liquid metals are overwhelmingly strong at conducting it (k). FLiBe has a higher ρcₚ than water but a high viscosity, so its index is 3.5. Gases have a ρcₚ below 1/100 of water's, so they are run at high pressure to raise density and with a large ΔT. Because Ẇ ∝ ΔT−2.8, changing only ΔT brings an SFR (about 150 °C) down to 0.85, about the level of water (about 33 °C), and an HTGR (about 500 °C) down to about 15 (first-order approximation).

Nuclear properties and activation

Thermal-neutron absorption cross sections are H 0.332 b, D 0.00052 b, Na 0.53 b, Pb 0.17 b, and almost zero for He-4. Fast reactors must avoid moderation, so they use Na, Pb or He rather than hydrogen. Each coolant produces different activation products.

  • H₂O: O-16(n,p)N-16 (T½ 7.13 s, γ 6.13 MeV). It disappears within minutes of shutdown.
  • D₂O: D(n,γ)T (T½ 12.3 years). Tritium has to be managed.
  • Na: Na-24 (T½ 15.0 h, γ 1.37 and 2.75 MeV). This is why an intermediate sodium loop is used.
  • Pb-Bi: Bi-209(n,γ) → Po-210 (T½ 138 d, α).
  • FLiBe: tritium is produced from Li-6 and Li-7, so highly enriched Li-7 is needed.

What it means in a plant

Operating conditions by reactor type

Pressure-temperature map with the light-water saturation curve up to the critical point at 22.06 MPa and 373.9 C, bars for SCWR at 25 MPa, HTGR at 7 MPa from 250 to 750 C and AGR at 4 MPa from 290 to 640 C, a zoom on PWR at 15.5 MPa from 291 to 324 C with about 21 C bulk subcooling to Tsat 344.8 C, PHWR at 9.9 MPa from 266 to 310 C and BWR at 7.0 MPa and 286 C, a near-atmospheric band for SFR, LFR and MSR, and a photo of room-temperature samples of water, sodium, lead and FLiBe
Pressure–temperature operating map by coolant. Bars run from inlet to outlet at the representative pressure; the saturation curve is from IAPWS-IF97. The sample photo shows the materials at room temperature, not in their operating state.
Reactor typeCoolantModeratorPrimary pressureInlet → outlet [°C]Example
PWRH₂O (single phase)H₂O15.5 MPa290.6 → 323.9APR1400
BWRH₂O (boiling in core)H₂Oabout 7.0 MPasteam about 286 (saturated)Typical BWR
PHWRD₂O (pressure tubes)D₂O (calandria, low temperature and pressure)outlet header 10.0 MPa (abs)about 266 → 310CANDU-6
AGRCO₂Graphiteabout 4 MPaabout 290 → 640UK AGR
HTGRHeGraphite7 MPa250 → 750HTR-PM
SFR (LMFBR)NaNonenear atmosphericabout 395 → 545Superphénix
LFRPb (Pb-Bi)Nonenear atmosphericabout 420 → 540BREST-OD-300
MSRMolten fluoride saltGraphite or nonenear atmosphericoutlet 700–800GIF target

The saturation pressure of light water is 7.0 MPa at 286 °C, 10.0 MPa at 311 °C and 15.5 MPa at 344.8 °C (IAPWS-IF97). At 15.5 MPa with a hot-leg temperature of 323.9 °C, a PWR keeps about 21 °C of bulk subcooling to prevent bulk boiling. This is a separate quantity from the DNBR margin. As a result, the outlet temperature of water-cooled reactors is tied to around 330 °C, and their thermal efficiency stays at about 33–35 %. Liquid metals and molten salts have high boiling points and reach 500 °C or more near atmospheric pressure. They have no depressurization boiling after a break, but freezing and chemical reactions become the problems to solve.

Coolants of fast reactors, PWRs and HTGRs — pros and cons

H₂O (PWR)Na (SFR)He (HTGR)
AdvantagesCheap and mature, high ρcₚ, doubles as moderator, negative moderator and void feedbackAtmospheric-pressure operation, boiling point 883 °C, high k, little moderationChemically and neutronically inert, no phase change, 750 °C or more → efficiency and hydrogen production
DisadvantagesNeeds high pressure, limited outlet temperature, depressurization boiling in a LOCA, radiolysis and corrosionViolent reaction with water and air, Na-24, opaque, preheating against freezing at 98 °C, sodium void coefficient can be positive at the core centerLow ρcₚ → high pressure and large blowers, leaks easily, graphite oxidation if air or moisture gets in
Compensating designPressurizer, ECCSIntermediate loop, pool type, steam generator leak monitoringLow power density and graphite heat capacity for passive decay-heat removal

CO₂ (AGR) is cheap and runs hot, but graphite oxidation has to be managed. Pb does not react violently with water, but it is heavy and corrodes steel, so its oxygen concentration is controlled.

Light-water and heavy-water reactors

In a light-water reactor, H₂O serves as both coolant and moderator, and reactivity is controlled with boric acid. A heavy-water reactor (CANDU-6) separates the hot, high-pressure D₂O coolant (380 pressure tubes) from the cold, low-pressure D₂O moderator (calandria). Absorption in D is about 1/640 of that in H, so natural uranium can be used. The price is the cost of D₂O, tritium, and a small positive coolant void coefficient. The fundamental differences between CANDU and the PWR are the moderator, the fuel (natural vs enriched), pressure tubes vs a pressure vessel, on-power vs shutdown refueling, and the reactivity control and shutdown systems (SDS1 and SDS2).

The six Gen-IV systems

The six systems selected in the GIF technology roadmap (2002, updated 2014) are distinguished by their coolants: VHTR (He, 900–1,000 °C), GFR (He, 850 °C), SFR (Na, 500–550 °C), LFR (Pb, 480–570 °C), MSR (fluoride salt, 700–800 °C) and SCWR (supercritical water, 510–625 °C). Outlet temperatures follow the GIF comparison table and differ between sources. The common direction is to leave the light-water saturation curve for high temperature at low pressure (or supercritical conditions).

Regulatory and design criteria

Examples of internationally used design criteria:

  • 10 CFR 50 Appendix A (United States): GDC 10 (fuel design limits), GDC 11 (reactor inherent protection), GDC 14 (reactor coolant pressure boundary), GDC 33, 34 and 35 (coolant makeup, residual heat removal, emergency core cooling). They were written with light-water reactors in mind.
  • NRC RG 1.232 Rev. 0 (April 2018): principal design criteria for non-light-water reactors, giving ARDC adapted from the GDC plus SFR-DC and MHTGR-DC. For example, GDC 14, which assumes a high-pressure boundary, does not fit reactor types that operate near atmospheric pressure as written.
  • IAEA SSR-2/1 Rev. 1 (2016): contains design requirements for the reactor coolant system (Requirement 47 and others). It is mainly a water-cooled reactor standard and is applied in a graded manner to other types.
  • Recent developments: the Gen-IV roadmap update (2014) and the non-LWR design criteria (RG 1.232, 2018) changed the regulatory framing; coolant properties and the selection principles are unchanged.

Easily confused pairs

CoolantModerator
PurposeRemove and transport heatSlow down neutrons
Key indicatorsρcₚ, k, pumping power, boiling pointξ, slowing-down power ξΣs, moderating ratio ξΣs/Σa
Fast reactorsNa, Pb, HeNone
Storing heat (ρcₚ)Conducting heat (k)
StrongestFLiBe, waterNa
EffectLess flow and pumping powerSmaller cladding temperature difference

"Sodium stores heat better than water" is a wrong statement. Its thermal conductivity is about 120 times higher, but its volumetric heat capacity is about 1/4.

Key points at a glance

  1. Definition: a fluid that removes and transports core heat (in LWRs it is also the moderator).
  2. Thermal: high ρcₚ → less flow; high k → small cladding temperature difference.
  3. Hydraulic: low viscosity → low pumping power, Ẇ ∝ μ0.2/(ρ²cₚ2.8).
  4. Phase change: high boiling point → low-pressure operation (water needs 15.5 MPa); low melting point → no freezing.
  5. Nuclear: low σa; for fast reactors, little moderation (no hydrogen).
  6. Activation: low induced activity, short half-lives (N-16 7 s, Na-24 15 h, Po-210).
  7. Chemical: compatible with structures, no reaction with water or air, stable under radiolysis.
  8. Economy and safety: cheap, negative void coefficient, no fire or explosion.
  9. Examples: H₂O (PWR, BWR), D₂O (PHWR), CO₂ (AGR), He (HTGR, VHTR, GFR), Na (SFR), Pb (LFR), fluoride salt (MSR).
Sketch: pressure-temperature axes with the water saturation curve and critical point, a PWR point at 15.5 MPa and 324 C, a helium point at 7 MPa and 750 C, a near-atmospheric line for Na, Pb and salt, and a box listing six coolant requirements
Sketch: operating window and six coolant requirements (schematic, no scale).