Showing posts with label reactor. Show all posts
Showing posts with label reactor. Show all posts

Sunday, April 19, 2015

Nuclear Plant May Have Unsafe Steel

Subtitle:  France May Have Installed Unsafe Steel In Flamanville Reactor

Several recent articles, including this one from BBC (see link), and this from RT (see link) state that the new nuclear power plant under construction in France's Flamanville complex has reactor vessel components with high carbon content; making the steel weaker than it should be.  
EPR Reactor Vessel for Flamanville, France


From the BBC article:

"In a joint statement, Areva and EDF said new tests were under way on the "reactor vessel head and bottom".

"It said this followed initial tests which had shown "greater than average carbon content" - something French regulators said caused "lower than expected mechanical toughness" in the steel."

This nuclear plant is the new, 1600 MWe EPR design, or European Pressurized Reactor.  Another EPR is under construction at Olkiluoto, Finland.   The planned new reactor at UK's Hinkley Point is to also have the same EPR design.   

Not having access to the laboratory test reports for the reactor components at Flamanville, it is not possible to assess the problem.  However, a few comments are in order. 

First, what quality control measures are in place that would allow such steel to be fabricated and installed?   It would appear that French regulators are remiss in their duty to ensure only acceptable materials of construction are used. 

Next, what impacts will occur if (and when) the reactor is rejected as unsafe?  How long will a new reactor require for fabrication and installation?    What will be the cost impacts?  Will the plant be finished, or abandoned as hopelessly costly?   Alternatively, can the reactor be modified at this time and made safe?  What will be the cost and schedule impacts of such modifications?

Next, what impact will there be on future plants?  Is the reactor at Olkiluoto made of the same steel?  The Hinkley Point EPR reactors are also stated as made from the same steel.  

Roger E. Sowell, Esq. 
Marina del Rey, California USA

copyright (c) 2015 by Roger Sowell 

Wednesday, April 2, 2014

The Truth About Nuclear Power - Part Six

Subtitle: Nuclear plants are huge to reduce costs
In this series of articles on the truth about nuclear power plants, one focus area is the economics.  Others include safety, financing, water usage, different technologies, and a few more.  This article addresses a part of the excessive cost issue: why are nuclear power plants so huge?  One description of these plants is “cathedrals”.  For perspective, modern designs are  approximately 1100 MWe per reactor, however a French design has 1,600 MWe per reactor.   
Another reason for the articles on nuclear plant costs is the argument by nuclear proponents that the only reason the plants cost so much is the opposition and lawsuits brought by anti-nuclear groups.   That is simply not true, as these articles demonstrate. The very nature of a nuclear power plant design, its inherent features as part of using nuclear fuel for heat, requires more equipment, larger equipment, more costly alloys, longer construction times, and attendant costs for equipment inflation and financing interest.   Even without lawsuits, nuclear power plants remain the highest cost plants for baseload power production.  Several studies reach the same conclusion on this point.
This article delves into attempts to reduce costs by three aspects of economy of scale, 
1) where bigger is cheaper if a manufacturing process is based on a circle or sphere; 
2) where mass production reduces costs; and 
3) where a learning curve makes future projects more efficiently constructed, in theory, at least.   
Those are three of the elements of gains due to economy of scale.  Each is addressed in turn.
Economy of scale based on a circle or sphere
This takes advantage of the fact that a pipe or tube has a circular cross-section.  A pipe with double the diameter can carry four times the quantity compared to the original pipe.   Also, if one doubles a sphere’s diameter, it holds eight times the volume.  These basic facts of engineering are employed all over the world in process plants, refineries, power plants, chemical plants, and any other process where fluids are moved through pipes or stored in spheres.   To a lesser extent, material storage in cylindrical tanks also achieve economy of scale as the tank diameter increases.   
Over time, nuclear power plant designs have increased in output from 600 MW to 1000 MWe to 1200 MWe to 1600 MWe, all as measured in electrical output, MWe.   These increases in size were attempts to reduce costs through economy of scale.   It is appropriate to pause here, and consider that statement.  If, as nuclear proponents assert, nuclear power really is as cheap as 4 cents per kWh, or 6 cents, why would it be necessary for successive designs to be bigger and bigger, trying to drive down the costs of the power produced?  The very fact that modern designs are bigger than previous designs puts the lie to the cheap power argument. 
Since most of a nuclear power plant has fluids, steam or water, flowing through a pipe or some similar item based on a circular cross-section, the first economy of scale applies.  As examples, the major equipment includes cylinders for the reactor vessel, steam generator, steam condenser, and containment structure.  Steam turbines also are based on a horizontal cylinder.   All the pipes, pumps, fittings, and valves also are based on a cylinder.   To illustrate, a pipe carrying water at 7 feet per second, approximately 2 meters per second, can convey 22 cubic feet per second.  If the pipe diameter is doubled, with velocity maintained at 7 feet per second, the water volume goes up by a factor of four to 88 cubic feet per second.   Similarly, if one wishes to double the plant size, for example from 600 MWe to 1200 MWe, pipes can achieve double the flow with an increased diameter of only 1.4 times the original size.   If the initial pipe is 2 feet or 24 inches in diameter, the pipe size that is required for double the flow is only 34 inches in diameter.  This is significant because a 34 inch pipe usually will not cost double that of a 24 inch pipe, but will cost only about 30 percent more than the 24 inch pipe.  The cost savings occur throughout the plant, wherever equipment is based on a circular cross-section.
Similarly, the third level of containment required by the NRC, the containment structure, typically has a dome for the roof.  A dome is half of a sphere, and economy of scale applies here, too.  The result is a plant with twice the production capacity, but a containment structure that costs approximately 1.3 times that of a smaller, half-sized plant. 
However, one factor works against the gains afforded by economy of scale.  That factor is the low steam pressure and temperature produced in a modern nuclear reactor system.  This requires that more steam must be circulated to produce the same amount of power.  Therefore, all equipment must be larger: reactor, steam generators, steam turbines, condensers, pipes, pumps, cooling towers, everything except the generator and electrical transmission equipment.  This is due to the low-pressure, saturated steam that is inherent in the PWR design.  The steam has no superheat and cannot use supercritical pressures due to risk of large pipes bursting, or the pipes must have prohibitively expensive thick walls.   There are proposals to overcome this problem by burning natural gas in supplemental boilers to provide superheat to the steam.  However, nuclear proponents are very much against natural gas and shudder at the thought that their nuclear power plant must allow natural gas on the premises. 
Economy of scale from mass production
In this aspect of economy of scale, the cost of each unit of production decreases where a large number of units are produced.  This is a very old concept, perhaps starting with the assembly line and manufacturing cars.  Certainly, the concept applies in many manufacturing processes.  For nuclear power plants, with only approximately 400 plants in the entire world, built over several decades, there has never been much opportunity to achieve mass production.    One reason for this has been the lack of standardized designs.  If each design is unique, the unique parts must each have its own design, drawings, manufacturing process that may require special jigs, possibly its own transportation system, installation system, etc.   This includes the major equipment such as the reactor, steam generator, steam condenser, steam turbine, power generator, auxiliary systems, containment structure, and other items.  The cost of each plant, therefore, suffers from a lack of mass production.   In the US, this problem has long been recognized and an attempt was made to standardize the design of new plants.  The Westinghouse AP-1000 design is supposed to solve the unique design aspect, so that each new plant will use the same design.  This has yet to occur, as the first such plants are currently under construction in Georgia at the Vogtle power plant.  These are, by definition, first-of-a-kind in the US.   The Vogtle plant has many drawbacks and serious issues, which will be addressed in one or more future articles.   It is notable that the Vogtle plant is building two reactors adjacent to each other, where there is at least a minimal opportunity to employ a small form of mass production.  However, building two of an item is not much better than building only one.  It requires building many items to reduce costs substantially.
Economy of scale from a learning curve
The cost reductions from a learning curve applies to the second and subsequent projects, which attempt to apply the lessons learned from building the first project.  This aspect of economy of scale works fairly well at times, but only when the lessons learned are effectively transferred to the subsequent projects.  In some cases, even when the lessons are communicated, the subsequent project has unique aspects that cannot apply the lessons.  Different geography, site conditions, climate and weather, all are examples of potential reasons why lessons cannot be applied.   There may also be different construction companies with different business philosophies, different equipment used in construction, and many other reasons why lessons learned will not be applied.   As above, using the Vogtle plant as the example, the two reactors are being built next to each other, and on a schedule so that one plant should follow about two years behind the first.   This will allow the second plant to take advantage of lessons learned, from the learning curve experienced in building the first plant.
Conclusion
Nuclear power plants cost far too much to build due to their inherent design for use of nuclear fuel.  The plants are huge to try to reduce the costs by economy of scale.
It can be seen that nuclear power plants have attempted to reduce the very high costs of construction by designing and building larger plants, by building multiple reactors at the same site, and to apply lessons learned from recent plants to the new plants.  It is still an interesting question, why should any of this be necessary if nuclear power plants truly produce electric power at the lowest cost of any type of baseload plant?  Some nuclear advocates go even further, with the assertion that nuclear plants can also be used as load-following plants.  If the costs of nuclear power were truly as low as the advocates maintain, there would be no reason ever to employ the well-known strategies of economy of scale. 
Benefits and drawbacks from building smaller, modular plants will be addressed in a future article in the series.

Previous articles in The Truth About Nuclear Power series can be found at the following links.


Roger E. Sowell, Esq.

Marina del Rey, California


Tuesday, April 1, 2014

The Truth About Nuclear Power - Part Five

Subtitle: You Cannot Simply Turn Off a Nuclear Power Plant

Fission-based commercial nuclear power plants are expensive for many reasons, but the main reason is due to the fact that nuclear heat is not like fossil heat; it produces deadly radiation, and one can’t just turn it off very easily.   The additional expense is a prudent, carefully-weighed and negotiated response to those basic facts. 
Palo Verde Nuclear Plant
source: NRC

Not much has changed in nuclear engineering since I first studied it in undergraduate school more than forty years ago.  Put simply, the uranium atom is so large, so unstable, that not only does it emit high-energy particles itself, it will easily split when it receives a neutron from an outside source.  The splitting of the atom is known as fission.  When fission occurs, several more neutrons are released.  The additional neutrons can be absorbed by other uranium atoms, causing them to undergo fission in what is termed a chain reaction.  This is, of course, greatly simplified.  Detailed discussions are available in many textbooks and on the internet.
The great benefit of fission is the tremendous amount of heat released, according to the famous Einstein equation E = M C^2.  (energy equals the mass times the speed of light, C, squared).    One of the great curses of nuclear fission is that heat must be removed as fast as it is produced, or many very bad things happen. 
In sharp contrast to gas-fired, oil-fired, or coal-fired power plants, which can be shut off easily and quickly, nuclear power plants cannot be easily shut off.  A nuclear reactor, once it has begun the fission process, continues to emit heat for a long time.  This residual heat must be removed to prevent the dreaded nuclear melt-down.  Nuclear industry proponents insist to this day that their plants are safe, they are designed with multiple safety systems, they are operated safely, they are routinely inspected and tested, and a melt-down will not happen.  Yet, we have seen clear evidence of reactor melt-downs; they have indeed happened.  The most infamous is probably the multiple-reactor melt-downs in Japan at the Fukushima complex.  But, one reactor in the US also suffered a partial melt-down, that one being the Three Mile Island plant.  (see link)   Back to the heat emitted and melt-downs, the safety systems are there to ensure the heat is removed.  
Perhaps it will be useful to go into some detail on how a nuclear reactor is designed and constructed, with a view toward why the multiple safety systems are required, and how this increases the construction cost.   A modern nuclear plant designed to meet the US Nuclear Regulatory Agency (NRC) requirements must have three levels of containment.  Containment is the word used to describe a physical barrier between the nuclear fuel pellets and the atmosphere.   The first containment is the fuel rod, a long metal cylinder that contains the nuclear pellets.  The pellets are short cylinders, roughly the size of the tip of a man’s index finger.  The metal walls of the fuel rod serve as the first containment.   The metal rods are made of an expensive alloy known as zircalloy.    From the NRC website, a fuel pellet is “[a] thimble-sized ceramic cylinder, 3/8 inches diameter by 5/8 inches long, consisting of uranium (typically uranium oxide, UO2), which has been enriched to increase the concentration of uranium-235 to fuel a nuclear reactor.  Modern reactor cores may contain 10 million pellets, stacked in the fuel rods that form fuel assemblies.”  see link  
The fuel rods are grouped in what is known as a fuel assembly, and multiple fuel assemblies are placed in the second containment, the reactor vessel.  The reactor vessel is a vertical metal cylinder with a bottom and top, made of thick alloy steel.   The reactor vessel is made of thick metal to withstand high temperatures and high pressures when the plant is operating.    The reactor vessel is very expensive, due to the wall thickness and the metal alloy.  There are also various pipes that must be connected to the reactor vessel, therefore the reactor wall has holes cut into it and short pieces of pipe and flanges welded onto it.  The fabrication of such a vessel is quite expensive.
Finally, the third containment is a reinforced-concrete room with a domed ceiling in which the reactor vessel and other plant equipment are placed.  The containment structure, as it is called, is “a gas-tight shell or other enclosure around a nuclear reactor to contain fission products that otherwise might be released to the atmosphere in the event of an accident.  Such enclosures are usually dome-shaped and made of steel-reinforced concrete.”  (NRC glossary)   The containment structure is also made of thick walls, floor, and ceiling.  Note the requirement that the containment structure be gas-proof.   The requirement for an enclosure, thick walls made of steel-reinforced concrete, and the gas-proof feature also makes the nuclear power plant very expensive.
Having now looked at the three levels of containment, fuel rods, reactor vessel, and containment structure, all made of expensive materials and by expensive methods, one can contrast this with a gas-fired power plant’s heat source.   In a steam plant, natural gas is piped to a boiler, where the gas is burned inside the boiler.  The boiler is typically a vertical, square or rectangular box with openings to allow air to flow into it, and an opening at the top to allow the gases formed from combustion to flow into the atmosphere.  That’s it.  There are no special alloy rods, no thick-walled alloy reactor, but there is a walled combustion chamber.   The combustion chamber, or boiler, has a compound wall that typically has an inner layer made of refractory to reflect and radiate heat back into the combustion chamber, a layer of insulation outside that, and a weather-resistant outer layer. 
A combustion turbine gas power plant is even simpler: the gas is piped into a small combustion chamber where it is mixed with compressed air and burned.  The hot combustion gases then flow through the blades of a power turbine, and from the exit of the power turbine, either into the atmosphere or into a heat-recovery steam generator. 
When one wants to shut down a gas-fired power plant, one simply shuts the valve that the natural gas flows through.  That’s it.  The fire goes out, the system begins to cool down.  Typically, water is pumped through the boiler tubes for some time to prevent the tubes from overheating, but this does not take long. 
To summarize to this point, the nuclear plant has millions of uranium fuel pellets stacked in individual rods, mainly to keep the pellets away from each other to prevent melt-downs.  The rods are enclosed in the reactor vessel that is very thick to withstand the temperature and pressure of the water that flows past the rods.  The flowing water removes the heat from the rods.  The containment structure is there “just in case” either of the first two containments fail and radioactive gases, steam, or liquids escape. 
It is the close proximity of millions of uranium fuel pellets that have split uranium atoms and produce various forms of radiation and heat that causes the next expensive safeguards.  If a nuclear reactor suffers a loss of reactor coolant, then bad things happen.  This situation is so important, the NRC has a special acronym for a Loss Of Coolant Accident, LOCA.  Much research has been conducted (see link) and thousands of pages have been written on LOCA.  The primary reactor coolant, as mentioned above, is flowing water that is pumped into the reactor and flows past the rods.  The rods are submerged in the water.  The hot water flows out of the reactor and is piped to one or more steam generators.  The steam generator is somewhat analogous to a gas-fired boiler’s steam separator drum.  However, the nuclear steam generator is far more expensive.  The steam generator is a vertical, U-tube heat exchanger with the hot water from the reactor on the tube side (flows through the U-tubes), and water and steam for the turbine on the shell side (flows past the U-tubes). 
More expense is required because a nuclear reactor of the pressurized water design as described, the modern design, has two separate water loops and separate pumping systems for each loop.  A gas-fired boiler has only one water loop and one set of pumps.  However, to be fair, an older design of nuclear reactors also has only one water loop, that is the boiling water reactor design.  But, modern designs use the pressurized water reactor with its two separate water loops.  The first water loop circulates water from the reactor to the steam generator, through a pump and back to the reactor.  The second water loop circulates water through the shell side of the steam generator where steam is produced, the steam flows through the turbine, through the condenser where it returns to water, then through a pump and back to the steam generator. 
The LOCA issue is so serious, the NRC also requires a reactor auxiliary cooling system, in case the primary cooling loop (the first water loop described above) fails.   The auxiliary cooling system requires more pumps, piping, valves, and a means to remove the reactor heat. 
Still more expense is required for the water pressurizer, the spent and fresh fuel storage areas, the spent fuel cooling system, and others.   None of these systems are required for a gas-fired power plant.
Conclusion
One reason nuclear power plants are so expensive is the nature of the fuel, uranium undergoing fission, can and does create deadly materials that must be contained within the reactor system.  Secondly, the plant cannot be shut down quickly.  The heat generated by the nuclear pellets is so intense that multiple provisions must be made to keep the fuel rods cool, keep the pellets from melting the rods and causing a melt-down.  The concern over a failure of the primary coolant system, LOCA, requires an expensive, redundant auxiliary cooling system.  The entire system could fail, which requires the expensive containment structure.   The inability to simply stop the heat, as by shutting a valve on the gas line in a gas-fired plant, requires that cooling systems continue to operate after the reactor is nominally shut down.  Residual heat continues to be generated by the fuel pellets.  A cooling system is required for the spent fuel storage area also. 
Additional reasons for the high cost of nuclear power plants will be discussed in future articles.  Such reasons include over-sized equipment, economies of scale, large commercial aircraft collision, and the high water consumption due to the nature of a nuclear reactor system. 
Previous articles in the Truth About Nuclear Power series are found at the following links.  Additional articles will be linked as they are published. 
Part Four – Nuclear Power Plants Use Far More Fresh Water





Roger E. Sowell, Esq.
Marina del Rey, California