Nuclear Fission
Releases energy by splitting heavy atomic nuclei (uranium, plutonium), converting mass to energy via E=mc² with ~3 million times the energy density of fossil fuels.
Fundamental Principle
The Fission Reaction
Nuclear fission releases energy by splitting heavy atomic nuclei into lighter fragments. When a neutron strikes a fissile nucleus (typically uranium-235 or plutonium-239), the nucleus becomes unstable and splits into two medium-mass fragments, releasing additional neutrons and enormous energy.
A typical U-235 fission reaction:
The exact fission products vary statistically, but the energy release is consistently around 200 MeV per fission event.
Energy Accounting
The ~200 MeV released per U-235 fission distributes approximately as:
| Component | Energy (MeV) | Recovery |
|---|---|---|
| Kinetic energy of fission fragments | 165 | Captured as heat |
| Kinetic energy of neutrons | 5 | Captured as heat |
| Prompt gamma rays | 7 | Captured as heat |
| Beta particles from fission product decay | 7 | Captured as heat |
| Gamma rays from fission product decay | 6 | Captured as heat |
| Antineutrinos | 10 | Lost (escapes reactor) |
| Total | ~200 | ~190 MeV recoverable |
Converting to macroscopic quantities:
- Energy per fission: 3.24 × 10⁻¹¹ J
- Energy per kg of U-235: 83.14 TJ/kg (theoretical complete fission)
- Practical energy per kg of fuel: ~45 TJ/kg (accounting for incomplete burnup)
Comparison with Chemical Energy
The energy density advantage of nuclear fuel over chemical fuels is extraordinary:
| Fuel | Energy Density | Ratio to Coal |
|---|---|---|
| Coal | 24 MJ/kg | 1× |
| Natural gas | 55 MJ/kg | 2.3× |
| Gasoline | 46 MJ/kg | 1.9× |
| Uranium (LWR, once-through) | ~500,000 MJ/kg | ~20,000× |
| Uranium (breeder cycle) | ~80,000,000 MJ/kg | ~3,000,000× |
A single uranium fuel pellet (about 7 grams) contains energy equivalent to approximately:
- 17,000 cubic feet of natural gas
- 1,780 pounds of coal
- 149 gallons of oil
This extreme energy density is nuclear power's fundamental advantage: enormous energy from minimal fuel mass, minimal mining, and minimal waste volume (though waste toxicity remains a challenge).
The Chain Reaction
For practical energy production, fission must be self-sustaining. Each fission releases 2-3 neutrons on average. If at least one neutron from each fission causes another fission, the reaction continues.
Criticality conditions:
- Subcritical (k < 1): Reaction dies out
- Critical (k = 1): Reaction sustains at constant rate
- Supercritical (k > 1): Reaction accelerates
Power reactors operate at criticality (k = 1), with the reaction rate controlled by:
- Control rods: Neutron-absorbing materials (boron, cadmium, hafnium) inserted to absorb excess neutrons
- Moderator: Material that slows neutrons to increase fission probability
- Delayed neutrons: ~0.65% of fission neutrons are emitted with delay (seconds), providing time for control adjustments
Without delayed neutrons, reactor control would be impossible, as the neutron generation time is microseconds.
Neutron Moderation
Fission neutrons emerge "fast" (energies >1 MeV, velocities ~10⁷ m/s), but U-235 has a much higher fission cross-section for "thermal" neutrons (energies ~0.025 eV, velocities ~2,200 m/s).
Moderator materials slow neutrons through elastic collisions:
- Light water (H₂O): Most common; also absorbs some neutrons, requiring enriched fuel
- Heavy water (D₂O): Better moderator (less absorption); allows natural uranium fuel
- Graphite: Solid moderator; used in some older designs
The moderation ratio (slowing power/absorption) determines how efficiently a moderator thermalizes neutrons without losing them.
Conversion Mechanism
Reactor Design Principles
Nuclear reactors convert fission heat to electricity through a thermodynamic cycle, typically a steam Rankine cycle:
- Fission releases heat in fuel
- Coolant (water, gas, or liquid metal) removes heat from fuel
- Steam generator (or direct boiling) produces steam
- Turbine converts steam energy to mechanical rotation
- Generator converts rotation to electricity
- Condenser rejects waste heat to environment
The thermal efficiency is limited by the Carnot efficiency and practical temperature constraints:
Nuclear plants typically operate at lower temperatures than fossil plants due to materials limitations, yielding lower thermal efficiencies.
Major Reactor Types
Pressurized Water Reactor (PWR) - ~70% of global fleet
- Coolant: Light water at ~155 bar, 290-325°C
- Moderator: Same water (separate from steam cycle)
- Fuel: Low-enriched uranium (3-5% U-235), UO₂ pellets
- Steam generation: Secondary loop (steam generators)
- Thermal efficiency: ~33%
- Examples: Westinghouse AP1000, French EPR, Russian VVER
Boiling Water Reactor (BWR) - ~15% of global fleet
- Coolant: Light water at ~75 bar, boiling at ~285°C
- Moderator: Same water
- Fuel: Low-enriched uranium (2.5-3.5% U-235)
- Steam generation: Direct (water boils in reactor vessel)
- Thermal efficiency: ~32%
- Examples: GE-Hitachi ABWR, ESBWR
Pressurized Heavy Water Reactor (PHWR/CANDU) - ~5% of global fleet
- Coolant: Heavy water (D₂O) at ~100 bar
- Moderator: Heavy water (separate system)
- Fuel: Natural uranium (0.7% U-235)
- Advantage: No enrichment required; online refueling
- Thermal efficiency: ~29-31%
- Examples: CANDU-6 (Canada), Indian PHWRs
Advanced Gas-cooled Reactor (AGR) - UK only
- Coolant: Carbon dioxide at ~40 bar, up to 650°C
- Moderator: Graphite
- Fuel: Enriched uranium (2.5-3.5%)
- Thermal efficiency: ~41% (highest of commercial reactors)
- Limited to UK; being phased out
Light Water Graphite Reactor (RBMK) - Russia/former USSR
- Coolant: Light water (boiling)
- Moderator: Graphite
- Fuel: Low-enriched uranium
- Design has positive void coefficient (safety concern)
- Chernobyl was RBMK; no new construction
Thermal Efficiency Comparison
| Reactor Type | Steam Temperature | Thermal Efficiency |
|---|---|---|
| PWR | 275-290°C (saturated) | 32-34% |
| BWR | 285°C (saturated) | 32-33% |
| PHWR (CANDU) | 260-310°C | 29-31% |
| AGR | 540-640°C (superheated) | 40-41% |
| Supercritical fossil | 540-620°C | 42-45% |
| Combined cycle gas | N/A | 55-62% |
Nuclear plants have lower thermal efficiency than modern fossil plants primarily due to:
- Fuel cladding temperature limits (zirconium alloys)
- Reactor vessel integrity requirements
- Safety margins for loss-of-coolant scenarios
Advanced reactor designs (Generation IV) aim for higher temperatures and efficiencies.
Capacity Factors
Nuclear plants excel at baseload operation with very high capacity factors:
| Technology | Typical Capacity Factor |
|---|---|
| Nuclear (US fleet 2024) | 92% |
| Nuclear (global average) | 80-82% |
| Coal | 40-50% |
| Combined cycle gas | 40-60% |
| Onshore wind | 25-35% |
| Solar PV | 10-25% |
| Hydropower | 30-50% |
The US nuclear fleet's 92% capacity factor represents decades of operational optimization. This high availability partially compensates for lower thermal efficiency in overall economics.
Fuel Cycle
Uranium Supply Chain
Mining:
Milling:
- Chemical extraction produces "yellowcake" (U₃O₈)
- ~85% uranium oxide content
Conversion:
- U₃O₈ converted to uranium hexafluoride (UF₆) for enrichment
- Gaseous UF₆ enables isotope separation
Enrichment:
- Natural uranium: 0.7% U-235, 99.3% U-238
- LWR fuel requires: 3-5% U-235
- Weapons grade: >90% U-235
- Methods: Gas centrifuge (dominant), gaseous diffusion (obsolete)
- Measured in Separative Work Units (SWU)
Fuel fabrication:
- Enriched UF₆ converted to UO₂ powder
- Pressed into ceramic pellets (~10 mm diameter, 10 mm height)
- Loaded into zirconium alloy tubes (fuel rods)
- Assembled into fuel assemblies (17×17 rod arrays typical for PWR)
Uranium Resources
Global identified recoverable uranium resources (2023):
- 7.9 million tonnes at <$260/kg U
- ~6 million tonnes at <$130/kg U
At current consumption (~67,000 tonnes/year):
- Known resources: ~90-120 years supply
- Including undiscovered resources: ~230 years
- With reprocessing and breeders: 3,000-30,000 years
- Seawater extraction (4.5 billion tonnes): effectively unlimited
Top countries by uranium resources (2023):
| Country | Resources (kt U) | Share |
|---|---|---|
| Australia | 1,684 | 28% |
| Kazakhstan | 906 | 15% |
| Canada | 588 | 10% |
| Russia | 486 | 8% |
| Namibia | 470 | 8% |
| South Africa | 320 | 5% |
| Brazil | 277 | 5% |
| Others | 1,204 | 20% |
Spent Fuel and Waste
A typical 1 GW PWR produces annually:
Spent fuel composition:
- ~95% uranium (mostly U-238)
- ~1% plutonium
- ~4% fission products and minor actinides
Waste management options:
Once-through cycle (most countries):
- Spent fuel stored in pools, then dry casks
- Eventual deep geological disposal
- US Yucca Mountain (canceled), Finland Onkalo (under construction)
Closed cycle with reprocessing (France, Russia, UK, Japan, India):
- Separates uranium and plutonium for recycling
- Reduces waste volume by ~75%
- Produces MOX fuel (mixed oxide)
- Reduces long-lived actinides
Advanced fuel cycles (future):
- Fast reactors could "burn" transuranics
- Thorium cycle produces less long-lived waste
Radioactive waste categories:
- High-level waste (HLW): Spent fuel, reprocessing liquids; requires isolation for 10,000+ years
- Intermediate-level waste (ILW): Reactor components, resins
- Low-level waste (LLW): Clothing, tools, filters
Nuclear produces far less waste by volume than fossil fuels, but waste toxicity and longevity remain significant challenges. A lifetime's electricity for one person from nuclear produces about 40 grams of high-level waste.
Global Status
Installed Capacity (2024-2025)
Global totals:
- Operating reactors: ~440
- Operating capacity: ~395-400 GWe
- Electricity generated (2024): ~2,670 TWh (record high)
- Share of global electricity: ~10%
Top countries by nuclear capacity:
| Country | Reactors | Capacity (GWe) | Nuclear Share |
|---|---|---|---|
| United States | 94 | 97 | 19% |
| France | 57 | 63 | 65-70% |
| China | 57 | 55 | 5% |
| Russia | 36 | 27 | 20% |
| South Korea | 26 | 26 | 30% |
| Canada | 19 | 14 | 15% |
| Ukraine | 15 | 13 | ~55% |
| Japan | 12 operating | 10 | 8% |
| India | 24 | 9 | 3% |
| UK | 9 | 6 | 15% |
Top 5 countries account for 71% of global nuclear capacity.
Construction and Pipeline
Under construction (2024-2025):
- ~63-70 reactors globally
- ~66 GWe total capacity
- Majority in China (29 units), India (6), Russia (4)
Construction starts (2024):
- 9 reactors began construction
- 6 in China, 1 each in Egypt, Pakistan, Russia
Countries building first reactors:
- Bangladesh: 2 units under construction
- Egypt: 4 units under construction
- Turkey: 4 units planned
Construction times:
- China average: 5-6 years
- Global average: 7-10 years
- Western projects often exceed 10 years (Vogtle, Flamanville, Olkiluoto)
Generation Trends
Nuclear electricity generation has been relatively stable:
- 1990: 2,013 TWh
- 2000: 2,591 TWh
- 2010: 2,756 TWh
- 2019: 2,796 TWh (pre-pandemic peak)
- 2022: 2,546 TWh (post-Fukushima low)
- 2024: 2,667 TWh (new record)
The 2024 record reflects:
- French fleet recovery from maintenance issues
- Chinese capacity additions
- Return of some Japanese reactors
Country Trajectories
Expanding:
- China: 57 operating, 29 under construction; targeting 70 GW by 2025, potentially 150 GW by 2035
- India: 24 operating, 6 under construction; plans for rapid expansion
- Russia: Domestic expansion plus major export program (Rosatom)
- United Arab Emirates: 4 units (5.4 GW) operational by 2024, first Arab nuclear program
Stable/Declining:
- United States: Aging fleet (average age ~42 years); some retirements offset by life extensions; Vogtle 3&4 completed 2023-2024
- France: Fleet aging; EPR Flamanville finally operational 2024; plans for 6 new EPR2 reactors
- Japan: 12 of 33 operable reactors restarted post-Fukushima; slow restart process
- UK: AGRs retiring; Hinkley Point C under construction (massive delays/cost overruns)
Phased out:
- Germany: Closed last 3 reactors April 2023; complete exit
- Italy: Exited 1990 after referendum
- Belgium: Phase-out extended to 2035 (from 2025)
Economics
Cost Components
Nuclear power costs divide into:
Capital costs (60-75% of LCOE):
- Reactor and containment construction
- Site preparation and grid connection
- Financing costs (interest during construction)
Operations and maintenance (15-25%):
- Staffing (large workforce required)
- Maintenance and inspections
- Regulatory compliance
Fuel costs (5-15%):
- Uranium purchase
- Conversion, enrichment, fabrication
- Spent fuel management
Decommissioning and waste (5-10%):
- End-of-life reactor dismantling
- Long-term waste storage/disposal
Levelized Cost of Electricity (LCOE)
LCOE estimates vary enormously depending on assumptions and location:
New nuclear construction (2024 estimates):
| Source | Region | LCOE ($/MWh) |
|---|---|---|
| Lazard | USA (Vogtle-based) | $142-222 |
| IEA/NEA | OECD average (7% discount) | $42-102 |
| BloombergNEF | China | $62 |
| BloombergNEF | USA | $180+ |
| IEA/NEA | Russia | $27-57 |
For comparison (2024):
- Onshore wind: 50)
- Utility solar: 61)
- Offshore wind: $72-140/MWh
- Natural gas combined cycle: $39-101/MWh
- Coal: $69-168/MWh
Existing nuclear plants (operating, depreciated) have very low marginal costs: $25-40/MWh, making continued operation economically attractive.
The Cost Challenge
Nuclear construction costs have increased dramatically in Western countries:
Overnight capital costs ($/kW):
- 1970s-1980s: $1,000-2,000
- 2000s: $2,000-4,000
- 2020s (Western): $6,000-15,000+
- China (2020s): $2,500-3,500
Contributing factors:
- Increased safety requirements (post-Three Mile Island, Chernobyl, Fukushima)
- First-of-a-kind engineering for new designs
- Loss of construction expertise and supply chains
- Regulatory complexity and delays
- Quality control issues causing rework
- Single-project, custom construction vs. serial production
Recent Western projects:
- Vogtle 3&4 (USA): 16,000/kW), 7+ year delays
- Hinkley Point C (UK): £34 billion for 3.2 GW (~$13,000/kW), years behind schedule
- Flamanville EPR (France): €19 billion for 1.6 GW (~$12,000/kW), 12+ year delay
- Olkiluoto 3 (Finland): €11 billion for 1.6 GW, 14 years construction
China's advantage:
- Serial construction of standardized designs
- Experienced workforce building multiple units simultaneously
- Lower labor costs
- Shorter regulatory timelines
- Result: 5-6 year construction, $2,500-3,500/kW
Economic Outlook
Nuclear faces a challenging economic environment:
- Competes with falling renewable costs
- High capital costs and long construction times increase financing risk
- Wholesale electricity prices often too low to justify new build
- Requires policy support (capacity payments, carbon pricing, clean energy credits)
However, nuclear offers value not captured in simple LCOE:
- Dispatchable, firm capacity (available on demand)
- No storage required for continuous operation
- Very high capacity factors
- Long operating life (60-80 years with extensions)
- Low lifecycle carbon emissions
Many analysts argue that "system LCOE" including storage and grid integration costs would favor nuclear, but this remains debated.
Advanced Reactors
Generation III+ (Current New Builds)
Currently deployed advanced designs:
Westinghouse AP1000:
- 1,117 MWe PWR
- Passive safety systems (no operator action for 72 hours)
- Modular construction
- Deployed: China (4 units), USA (Vogtle 3&4)
EPR (European Pressurized Reactor):
- 1,650 MWe PWR
- Four-train safety systems
- Core catcher for severe accidents
- Deployed: China (2), Finland (1), France (1 in 2024)
Russian VVER-1200:
- 1,200 MWe PWR
- Exported widely (Belarus, Bangladesh, Egypt, Turkey, India)
- Rosatom's export workhorse
APR1400 (South Korea):
- 1,400 MWe PWR
- Deployed in UAE (4 units, Barakah)
- Competitive construction costs
Small Modular Reactors (SMRs)
SMRs are reactors under 300 MWe designed for factory fabrication and modular deployment.
Operational SMRs (as of 2024):
| Reactor | Country | Capacity | Status |
|---|---|---|---|
| Akademik Lomonosov | Russia | 2×35 MWe | Floating, operational 2020 |
| HTR-PM | China | 2×105 MWe | Pebble-bed, grid 2021 |
| RITM-200 | Russia | 55 MWe | Icebreakers |
Leading SMR designs in development:
NuScale VOYGR (USA):
- 77 MWe per module (up to 6 modules)
- First SMR design certified by US NRC (2022, 2025 uprate)
- First US project (UAMPS) canceled November 2023 due to cost escalation
- International projects under development (Romania, Poland, others)
- Estimated LCOE: $89-119/MWh (higher than large reactors)
GE-Hitachi BWRX-300:
- 300 MWe simplified BWR
- Natural circulation, passive safety
- Targeting coal plant replacement
- Projects in Poland, Canada, Romania
Rolls-Royce SMR (UK):
- 470 MWe PWR
- Factory-built modules
- Selected for UK Wylfa site
- Targeting mid-2030s deployment
Terrestrial Energy IMSR (Canada):
- 190 MWe molten salt reactor
- Higher temperature for industrial heat
- In licensing process
SMR challenges:
- Economies of scale work against smaller units
- First-of-a-kind costs remain high
- "Nth of a kind" savings require large order books
- NuScale UAMPS cancelation highlighted cost concerns
- CSIRO estimated SMR electricity 2.5× cost of large reactors
SMR potential advantages:
- Smaller upfront investment
- Faster construction
- Flexible siting (smaller footprint, lower cooling needs)
- Load-following capability
- Industrial heat applications
Generation IV Reactors
Six advanced reactor concepts under international development:
Sodium-cooled Fast Reactor (SFR)
- Liquid sodium coolant, fast neutron spectrum
- Can breed fuel and burn actinides
- TerraPower Natrium (USA) under construction
- Russian BN-800 operational
Lead-cooled Fast Reactor (LFR)
- Liquid lead or lead-bismuth coolant
- High temperature capability
- Newcleo (UK/Italy) in development
Molten Salt Reactor (MSR)
- Fuel dissolved in molten salt coolant
- Inherent safety (fuel drains to dump tank)
- Can use thorium fuel cycle
- Terrestrial Energy, Kairos Power developing
Very High Temperature Reactor (VHTR)
- Helium coolant, graphite moderator
- 750-1000°C outlet temperature
- Process heat for hydrogen production
- China HTR-PM partially demonstrates
Supercritical Water-cooled Reactor (SCWR)
- Water above critical point (374°C, 22 MPa)
- Higher thermal efficiency (~45%)
- Conceptual stage
Gas-cooled Fast Reactor (GFR)
- Helium coolant, fast spectrum
- Conceptual stage
Generation IV timeline:
- Most designs remain at demonstration stage
- Commercial deployment: 2030s-2040s (optimistic)
- Key barriers: Materials qualification, licensing frameworks, economics
Environmental Considerations
Lifecycle Emissions
Nuclear power has very low lifecycle CO₂ emissions:
| Technology | Lifecycle Emissions (g CO₂-eq/kWh) |
|---|---|
| Coal | 820 |
| Natural gas | 490 |
| Solar PV | 41 |
| Nuclear | 12 |
| Onshore wind | 11 |
| Hydropower | 24 |
Nuclear's emissions come primarily from:
- Uranium mining and milling
- Enrichment (if using fossil-powered electricity)
- Construction materials (concrete, steel)
- Decommissioning
The fuel cycle is far less carbon-intensive than any fossil fuel.
Safety Record
Major accidents:
Deaths per TWh (all causes):
| Energy Source | Deaths per TWh |
|---|---|
| Coal | 24.6 |
| Oil | 18.4 |
| Natural gas | 2.8 |
| Hydropower | 1.3 |
| Wind | 0.04 |
| Nuclear | 0.03 |
| Solar | 0.02 |
Nuclear is among the safest energy sources per unit of electricity generated, primarily because:
- Fuel is contained in multiple barriers
- Plants designed for beyond-design-basis accidents
- Regulatory oversight is intensive
Land Use
Nuclear has the smallest land footprint per unit of energy:
| Technology | Land Use (m²/MWh/year) |
|---|---|
| Nuclear | 0.3 |
| Natural gas | 0.4 |
| Coal | 1.0 |
| Solar PV | 5-10 |
| Wind | 70-100 (including spacing) |
| Hydropower | Variable (reservoir) |
A 1 GW nuclear plant occupies ~1-4 km². An equivalent solar farm requires ~15-25 km².
Water Use
Nuclear plants require significant cooling water (like all thermal plants):
- Once-through cooling: 100-200 m³/MWh (returned to source, warmer)
- Cooling towers: 2-3 m³/MWh consumed (evaporated)
This can constrain siting in water-scarce regions. Some advanced designs target air cooling or reduced water use.
Proliferation and Security
Nuclear power creates materials (enriched uranium, plutonium) with potential weapons applications:
Security concerns include:
- Terrorist attacks on facilities
- Theft of nuclear materials
- Sabotage
Modern plants are designed to withstand aircraft impact and other threats.
Strategic Outlook
Role in Decarbonization
Nuclear's potential contribution to climate mitigation:
IEA Net Zero Scenario:
- Nuclear doubles by 2050 (from ~400 GW to ~800 GW)
- Requires ~30 GW/year of new construction (vs. ~5-7 GW/year currently)
IPCC scenarios:
- Most 1.5°C pathways include nuclear expansion
- Range from modest growth to 500% increase by 2100
COP28 Declaration (2023):
- 31 countries committed to tripling nuclear capacity by 2050
- Would require ~1,200 GW by 2050
Near-Term Prospects (2025-2035)
Likely developments:
- China continues rapid expansion (5-8 units/year)
- Existing fleet life extensions in US, Europe, Japan
- SMR demonstration projects come online (or fail)
- Some new large reactor construction in Europe, Asia
Challenges:
- Cost competitiveness with renewables+storage
- Financing for capital-intensive projects
- Supply chain and workforce rebuilding in West
- Regulatory timelines
Realistic capacity by 2035:
- Low scenario: 420 GW (modest growth, retirements offset by new build)
- High scenario: 500 GW (successful new programs, life extensions)
Long-Term Potential
By 2050:
- Capacity range: 500-1,000 GW
- Depends critically on construction costs, policy support, public acceptance
- SMRs and advanced reactors could change economics (or not)
- Fusion remains unlikely to contribute before 2050
Key uncertainties:
- Can Western countries rebuild nuclear construction capability?
- Will SMRs achieve cost reductions through serial production?
- How will nuclear compete with renewables+storage?
- Will public acceptance increase or decrease?
- Can construction timelines and costs be controlled?
Comparative Assessment
| Attribute | Nuclear | Wind+Solar+Storage |
|---|---|---|
| Dispatchability | Excellent | Requires storage |
| Land use | Minimal | Significant |
| Capacity factor | 80-92% | 25-35% (before storage) |
| Construction time | 5-15 years | 1-3 years |
| Capital intensity | Very high | Moderate |
| Fuel supply security | High (small volume, stockpileable) | High (no fuel) |
| Public acceptance | Contested | Generally positive |
| Waste | Long-lived, low volume | Short-lived, high volume |
Nuclear and renewables are often framed as competitors, but both are needed for deep decarbonization. Nuclear provides firm, dispatchable power that complements variable renewables.
Conclusion
Nuclear fission offers an extraordinarily energy-dense, low-carbon power source that has operated safely and reliably for over 60 years. Its ~400 GW global capacity generates 10% of world electricity with minimal emissions, land use, and fuel requirements.
The technology faces genuine challenges:
- High capital costs and long construction times (especially in Western countries)
- Unresolved waste disposal (politically more than technically)
- Public concerns about safety and proliferation
- Competition from increasingly cheap renewables
Yet nuclear also offers unique advantages:
- Dispatchable, firm capacity requiring no storage
- Extremely high energy density and low material throughput
- Very low lifecycle emissions
- Long operating life (60-80 years)
- Minimal land footprint
The path forward likely involves:
- Continued operation and life extension of existing plants
- New construction primarily in Asia (China, India)
- SMR development (uncertain economics)
- Advanced reactor demonstration in 2030s
- Potential for significant role in decarbonization if costs can be controlled
Nuclear fission is neither the sole solution to climate change nor a technology that should be abandoned. It is a proven, scalable, low-carbon energy source whose future role will be determined by economics, policy choices, and societal preferences as much as by technical factors.