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Nuclear power

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Nuclear power
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UEET 603

Introduction to Energy Engineering

Spring 2010



Nuclear Power

•Nuclear energy is a way of creating heat through

the fission process of atoms.



•Nuclear energy originates from the fission of

atomic nucleus in a chain reaction.



•Nuclear fission reaction is controlled in a

nuclear reactor to produce thermal energy.

• The fission process takes place when the nucleus

of a heavy atom like uranium or plutonium is

split when struck by a neutron.



• The fission of the nucleus releases two or

more new neutrons.



• It also releases energy in the form of heat.



• The released neutrons can then continue to split

additional nucleus .

- This releases even more neutrons and more

nuclear energy.

- The repeating of the process leads to a chain

reaction.

• All nuclear power plants convert heat into electricity

using steam.

• The heat is created when atoms are split apart – called

fission.

• The heat from fission reaction is used to produce

steam, which is then used to turn a turbine and

produce electricity using a generator.

• Power from nuclear fission accounts for about 19% of

the nation’s total energy.

• Number of operating nuclear power plants is 120 ??

• Mostly safe, successful and well regulated

• No new power plant has been built in last 30 years

• Nuclear power is generated primarily in stationary

applications like in a nuclear power plants, propulsion of

mobile system like naval vessels, especially submarines as

well as several surface vessels.



• Since nuclear plants do not consume oxygen like

conventional plants, it is quite attractive for use under sea.



• Also, ships powered by nuclear plants need to be refueled

only after long period of operation.



• Nuclear power has also been developed for the propulsion

of aircrafts and rockets.

Safe operation of the plant and safe handling and disposal of

nuclear fuels.



Concern of environmentalists about the dangers of storing

the radioactive byproducts of the process.



Cost of building a new nuclear reactor is about $10 billion

each – One of the main reason for a stagnant industry.



Recent reduced cost of other fuels like coal, natural gas and

oil, make the nuclear power production less competitive.



Each project has to pass through a rigorous scrutiny and

check through Nuclear Regulatory Commission (NRC) before

construction can begin.

• Needs economic guarantee from the government



• Without any support from the government it seems

difficult for the utility companies to start any new projects.



• Government recently committed $8.33 billion

in loan guarantees for the construction of two

new reactors at the Alvin W. Vogtle Electric

Generating Plant in Georgia

- Expected to provide electricity to

over a million people by next 5-6 years.

- Expected to create new job opportunities.

Fundamental Particles



The physical world is composed of various subatomic or

fundamental particles.



There are variety of different fundamental particles, and

scientists are still finding newer ones .



However , only few of these are important in nuclear

engineering:



- Electrons - Proton - Neutron



- Photon - Neutrino

Electrons:

m  9.10956  10  28 g

• This particle has rest mass of e

and carries a charge e  1.60219 10 19 coulombs



• Mass of a particle is a function of its speed relative to the

observer



• In giving the mass of fundamental particle, it is necessary to

specify the mass at rest with respect to the observer -

termed as rest mass.

There are two types of electrons:

• Negatrons or negative electrons:

Carries a negative charge

Normal electrons encountered in this

world.

• Positrons or positive electrons:

Carries a positive charge

Relatively rare in this world

These two are identical except the sign of

the charge

Electron Annihilation Process

• When under circumstances, a positron collide

with a negatron, the electrons disappear and

two (occasionally more) photon (particles of

electromagnetic radiation) are emitted.

Proton

• 24

This particle has a rest mass of m p  1,6726110 g

and carries a positive charge equal in magnitude

to the charge on the electron.

• Protons with negative charge have also been

discovered, but these particles are of no

importance in nuclear engineering.

Neutron

• The mass of a neutron is mn  1.67492  10 24 g

which is slightly larger than the mass of the

proton.

• It is electrically neutral.



• The neutron is not a stable particle, except

when it is bound into an atomic nucleus.



• A free neutron decays to a proton with the

emission of a negative electron (Known as β  decay

)

Photon

• Particle equivalent of electromagnetic wave.

• This is a particle with zero rest mass and zero

charge, which travels in a vacuum at only one

speed, namely the speed of light c  2.0079  1010 cm/s

Neutrino

• This also a particle with zero rest mass and no electrical

charge.

• This appears in the decay of certain nuclei.

• There are two types of Neutrinos: neutrinos and

antineutrinos

Atoms are the building blocks of all gross matter



Atoms, in turn, consists of a small but massive nucleus

surrounded by a cloud of rapidly moving (negative)

electrons



The nucleus is composed of protons and neutrons



The total number of protons in the nucleus is called

the atomic number (Z) of the atom.

• Total electrical charge of the nucleus is : +Ze

• In a neutral atom there are as many electrons as

protons, i.e. Z-number of electrons moving around the

nucleus.



• It is the number electrons that dictates thechemical

behavior of atoms and gives identify of a element.



Hydrogen (H) has one electron

Helium (He) has two electrons

Lithium (Li) has three electrons



• The number of neutrons in a nucleus is known as

the neutron number (N)



Atomic mass number: A = Z+N

The various species of atoms whose nuclei contain

particular numbers of protons and neutrons are called

nuclides.



Each nuclides is denoted by the chemical symbol of the

element (this specifies Z) with the atomic mass number

as superscript.

This determines the number of neutrons N = A-Z

1

H : Hydrogen nuclide with ( Z=1) a single proton

as nucleus

2

H is the hydrogen nuclide with a neutron and as well

as a proton in the nucleus. This called the deuterium

of heavy hydrogen .

4

He is the helium nuclides whose nucleus consists

of two proton (two electron) and two neutrons.



For better clarity, Z is also included in the symbol

as a subscript.



Atoms such as 1 H and 2 H whose nuclei contains

same number of protons but different numbers of

neutrons ( Same Z but different N and hence

different A) are known as isotopes.



Naturally occurring elements may exist in the

nature with some stable isotopes and some

unstable isotopes and expressed as

percentage atoms of the element.

• Oxygen, for example, has three stable isotopes 16 O ,

17

O , 18O ( Z = 8, N = 8, 9 , 10 ) and five known unstable ( i.e.

20

radioactive) isotopes O , O , O , O and O (Z = 8, N=5, 6,

13 14 15 19



7, 11, 12).



• The stable isotopes ( and a few of the unstable isotopes) are

found as naturally occurring elements in nature.



• However, they are not found in equal amounts; some isotopes

of a given element are more abundant than others.

For example: 99.8 % of naturally occurring

oxygen atoms are the isotope 16 O . Rest are:

0.037% O and 0.204%

17

Einstein’s theory of relativity

• Mass and energy are equivalent and

convertible, one into other.



•Complete annihilation of a particle or other body

of rest mass m 0 releases an amount of energy

which is given by Einstein’s formula



E rest  m0 c 2



c is the speed of light

For example, the annihilation of 1g of matter would lead to a

release of



E  1 2.9979 10 

10 2

 8.9874 1020 erg  8.984 1013 joules

- This is equivalent to 25 million kilowatt-hours



Another unit of energy that is often used in nuclear engineering

is the electronVolt (eV)



This is defined as the increase in the kinetic energy of an

electron when it falls through an electrical potential of one volts.



This is in turn is equal to the charge of the electron multiplied by

the potential drop



1eV  1.60219 10 19 Coulomb  1 Volt  1.60219 10-19 Joule

When a body is in motion, its mass increases relative to

an observer according to the formula



m0

m

v2

1

c2





Total energy of a particle, that is, its rest mass plus its

kinetic energy





Etotal  mc2



Kinetic energy is given as

 



 1 

 For v<< c Same as in Classical

E  mc 2  m0 c 2  m0 c 

2  1 Mechanics

 1 v 



E  m0 v 2

 c2 

 2

Energy of Atomic particles

1

Neutron: E  m0 v 2 v  2.383  106 E

2



Photon: Travels at the speed of light and has no

rest mass, its total energy is given as

E  hv



Particle Wave Length

For Neutron

9 For Photon and all other

2.869  10

 particles of zero rest mass

E

1.240  10  4



Where E is the kinetic E

energy in eV

Excited States and Radiation

 The z atomic electrons that cluster about the nucleus

move in a well defined orbits

 However, some of these electrons are more tightly

bound in the atom than other.

 For example only 7.38 eV is required to remove the

outermost electron from a lead (Z=82), while 88 keV

(or 88,000 eV) is required to remove the inner most or

the k-electron.

 The process of removing an electron from an atom is

call ionization and 7.38 eV and 88k3V are known as

the ionization energies.

 This leads to a excited state for the atom –has more

energy than the ground state.

 It slow decays back to the ground state.

 When such transition occurs, a photon is emitted by

the atom with an energy equal to the difference in the

energies of the two states.

 Depending on the energy level of the excited state or

the removed electron orbit level, radiation wavelength

( ultraviolet etc. ) can be determined.

•Light -Water Reactor (LWR)

•Gas Cooled Graphite moderated Reactor

- High temperature gas cooled reactor (HTGR)



•Heavy -Water Reactor (HWR)

•Breeder Reactor (BR)

• The first generation of reactor that is There are two

moderated and cooled by ordinary (light) types of light

water.

- water

• Water has excellent moderating reactors:

properties as well as thermodynamic

properties to produce steam. Pressurized-

water reactor

• Water also absorbs neutrons to such an (PWR)

extent that it is not possible to fuel a LWR

with natural uranium – it simply would not

become critical. Boiling-water

reactor (BWR)

• Uranium in LWR must always be

enriched to some extent.

The water in a PWR is

maintained at a high pressure

in the range of 2000-2500 psi

Containment Structure to prevent water from boiling.

Steam

Control Generator High pressure water is

Rods circulated through the reactor

core to pick up heat without

any boiling of water.

Turbine

Pressurize hot water is then

Generator circulated through the steam

generator where heat is

transferred to a secondary

water stream that enters as

Condenser liquid water and exits steam.

Reactor Vessel

High pressure and high temperature steam is then turns

a turbine to produce electric power.



Large PWR system uses as many as four steam

generators, which produce steam at about 560 F and

900 psi.



This gives an overall efficiency of 32-33 % for a PWR

plant.



The condenser is cooled by a cooling water loop using

pumps and cooling tower that rejects heat to

environment

Boiling Water Reactor (BWR)

•Referred to as the direct cycle.

Containment Structure

•Water is boiled directly in the

Steam reactor vessel and produces

Control Generator steam to turn the turbine.

Rods



•Steam is produced directly

inside the reactor and there is

Turbine

no need of a separate steam

generator.

Generator



•Steam from the rector goes

directly to the turbine to

produce power.

Condenser



•More effective in removing

Reactor Vessel r



heat from the fission reaction

using latent heat rather than

sensible heat.

Less water is pumped through the reactor than a PWR

for the same net power output



However, the water becomes radioactive in passing

through the reactor core.



Since this radioactive water is utilized in the electricity

producing side of the plant, all of the components like

the turbines, condensers, reheaters, pumps, piping be

shielded in a BWR Plant.



The pressure in a BWR is approximate 1000 psi, about

half the pressure in a PWR.

As a results the wall of the pressure vessel for a BWR

need not be as thick as it is for a PWR.



However the power density (Watt/cm^2) is smaller in a

BWR than a PWR, and so overall dimension of a

pressure vessel for BWR must be larger than for PWR.

Heavy-Water ( D2O )Reactor

Heavy-water moderated and cooled reactor

(HWR) has been under development in several

countries, especially in Canada.



Heavy-water moderated reactor is suitable for use with

natural uranium.



Canada has large resources of natural uranium.



Removes the need for expansive uranium enrichment

plant.

•Such a reactor can operate on natural Uranium

because the absorption cross section of

deuterium ( D = 2 H ) for thermal neutron is very small,

much smaller for example than the cross section of

ordinary hydrogen ( H = 2 H ).



•However, deuterium in D2O is twice as heavy as

hydrogen in H 2 O, so that D2O is not as effective in

moderating neutrons as H 2 O .

•They require more collisions and travel greater

distances before reaching thermal energies than

H 2O

•The core of an HWR is therefore considerably larger

than that of an LWR, but much smaller than a natural

uranium, gas cooled graphite moderated reactor.



•In order to avoid the use of large and expensive

pressure vessel, Canadian design uses pressure tube

concept that encapsulated fuel within a hollow tubes.



•The coolant passes through the tubes and coolant do

not come in direct contact with the heavy water

moderator.



•In Canadian HWR design, heavy water is also used as

the coolant.

•One important thing about the HWR is that the reaction

is not inherently stable.



•Thus an accidental increase in power leads automatically

to further increase in power and rapid external

intervention is required to bring reactor under control

Breeder Reactor

• The world reserve of 235

U are not adequate to meet the

indefinite needs of the growing nuclear power industry ( may be

for 100 years)



•Only the advent of the breeder reactor can achieve the full

potential of the world’s uranium and thorium supply.



•It is possible to manufacture certain fissile isotopes from

abundant non-fissile materials by a process know an

conversion.

The two most important fissile isotopes produced from conversion

are 233 U and 239 .

Pu

The fissile isotope 233 U is obtained from fissile isotope 232

U of

thorium by the absorption of neutrons.





239

Pu is obtained from nonfissile 238 U , which is one of the major

component of natural resource of uranium.

238

U has to be irradiated in a reactor, which normally occurs in

most the reactors. So most of the reactor are fueled with uranium

which is only slightly enriched in 235 U .



Practically all of the fuel in these reactors is therefore 238 U and

conversion of 238 U into 239 Pu takes place during the normal

operation of the rector.

The conversion process is described in terms of conversion

ratio or breeding ratio

- Defined as the average number of fissile atoms

produced in a reactor per fissile fuel atom consumed.



In a breeder reactor every effort is made to prevent fission

neutrons to slow down. So, light-water is excluded from

the core.



There is no moderator in the core and the core contains

only fuel rods and coolant.



In these reactors, different other types of coolants such as

sodium are used.

Types of Breeder Rectors:



• Liquid-metal Cooled fast Breeder Rector

(LMFBR)



• Gas cooled fast breeder Reactor (GCFR)



• Molten salt breeder reactor (MSBR)



• Light water breeder reactor


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