## Law of Conservation of Energy

**The law of conservation of energy**is one of the basic laws of physics along with the

**conservation of mass**and the conservation of momentum.

**The law of conservation of energy**states that energy can

**change**from one

**form**into another, but it

**cannot be created or destroyed**. Or the general definition is:

The total energy of an isolated system remains constant over time.

**Energy** can be defined as the **capacity for doing work**. It may exist in a variety of forms and may be **transformed** from one type of energy to another in hundreds of ways.

For example, burning gasoline to power cars is an energy conversion process we rely on. The **chemical energy** in gasoline is** converted** to** thermal energy**, which is then converted to **mechanical energy** that makes the car move. The **mechanical energy** has been converted to **kinetic energy**. When we use the brakes to stop a car, that** kinetic energy** is converted by friction back to heat, or **thermal energy**.

A consequence of the law of conservation of energy is that a perpetual motion machine of the first kind, which produces work without the input of energy, cannot exist.

The concept of** energy conservation** is widely used in many fields. In this article the following fields are discussed:

**Conservation of Mechanical Energy****Conservation of Energy in Fluid Mechanics****Conservation of Energy in Thermodynamics**- Conservation of Energy in Electrical Circuits
- Conservation of Energy in Chemical Reactions
**Conservation of Energy in Special Relativity Theory****Conservation of Energy in Nuclear Reactions**

## Law of Conservation of Energy in Classical Physics

## Conservation of Mechanical Energy

**Conservation of Mechanical Energy**was stated:

**The total mechanical energy** (defined as the sum of its potential and kinetic energies) of a particle being acted on by only conservative forces** is constant**.

**An isolated system** is one in which **no external force** causes energy changes. If only **conservative forces** act on an object and **U** is the** potential energy** function for the total conservative force, then

**E**_{mech}** = U + K**

**The potential energy, U**, depends on the position of an object subjected to a conservative force.

It is defined as the object’s ability to do work and is increased as the object is moved in the opposite direction of the direction of the force.

**The potential energy** associated with a system consisting of Earth and a nearby particle is **gravitational potential energy**.

**The kinetic energy, K**, depends on the speed of an object and is the ability of a moving object to do work on other objects when it collides with them.

** K = ½ mv ^{2}**

The above mentioned definition (**E**_{mech}** = U + K**) assumes that the system is **free of friction** and other **non-conservative forces**. The difference between a conservative and a non-conservative force is that when a conservative force moves an object from one point to another, the work done by the conservative force is independent of the path.

In any real situation, **frictional forces** and other non-conservative forces are present, but in many cases their effects on the system are so small that the principle of **conservation of mechanical energy** can be used as a fair approximation. For example the frictional force is a non-conservative force, because it acts to reduce the mechanical energy in a system.

Note that non-conservative forces do not always reduce the mechanical energy. A non-conservative force changes the mechanical energy, there are forces that increase the total mechanical energy, like the force provided by a motor or engine, is also a non-conservative force.

**pendulum**(ball of mass m suspended on a string of length

**L**that we have pulled up so that the ball is a height

**H < L**above its lowest point on the arc of its stretched string motion. The pendulum is subjected to the

**conservative gravitational force**where frictional forces like air drag and friction at the pivot are negligible.

We release it from rest. **How fast is it going at the bottom?**

The pendulum reaches **greatest kinetic energy** and **least potential energy** when in the **vertical position**, because it will have the greatest speed and be nearest the Earth at this point. On the other hand, it will have its **least kinetic energy** and **greatest potential energy** at the **extreme positions** of its swing, because it has zero speed and is farthest from Earth at these points.

If the amplitude is limited to small swings, the period *T* of a simple pendulum, the time taken for a complete cycle, is:

where ** L** is the length of the pendulum and

**is the local acceleration of gravity. For small swings the period of swing is approximately the same for different size swings. That is,**

*g***the period is independent of amplitude**.

## The Law of Conservation of Energy – Nonconservative Forces

**nonconservative forces**such as friction, since they are important in real situations. For example, consider again the pendulum, but this time let us include

**air resistance**. The pendulum will slow down, because of friction. In this, and in other natural processes, the

**mechanical energy**(sum of the kinetic and potential energies)

**does not remain constant**but decreases. Because

**frictional forces**reduce the mechanical energy (but not the total energy), they are called

**nonconservative forces**(or

**dissipative forces**). But in the nineteenth-century it was demonstrated

**the total energy is conserved in any process**. In case of pendulum its initial kinetic energy is all transformed into thermal energy.

For each type of force, conservative or nonconservative, it has always been found possible to define a type of energy that corresponds to the work done by such a force. And it has been found experimentally that **the total energy E** always remains constant. The **general law of conservation of energy** can be stated as follows:

*The total energy E of a system (the sum of its mechanical energy and its internal energies, including thermal energy) can change only by amounts of energy that are transferred to or from the system.*

## Conservation of Momentum and Energy in Collisions

The use of the **conservation laws for momentum and energy** is very important also in **particle collisions**. This is a very powerful rule because it can allow us to determine the results of a collision without knowing the details of the collision. The law of **conservation of momentum** states that in the collision of two objects such as billiard balls, the **total momentum is conserved**. The assumption of conservation of momentum as well as the conservation of kinetic energy makes possible the calculation of the **final velocities** in two-body collisions. At this point we have to distinguish between two types of collisions:

**Elastic collisions****Inelastic collisions**

## Elastic Collisions

**perfectly elastic collision**is defined as one in which there is

**no net conversion of kinetic energy**into other forms (such as heat or noise). For the brief moment during which the two objects are in contact, some (or all) of the energy is stored momentarily in the form of

**elastic potential energy**. But if we compare the total kinetic energy just before the collision with the total kinetic energy just after the collision, and they are found to be the same, then we say that the

**total kinetic energy is conserved**.

- Some large-scale interactions like the
**slingshot type gravitational interactions**(also known as a planetary swing-by or a gravity-assist manoeuvre) between satellites and planets are**perfectly elastic**. - Collisions between
**very hard spheres**may be**nearly elastic**, so it is useful to calculate the limiting case of an elastic collision. - Collisions in
**ideal gases**approach perfectly elastic collisions, as do scattering interactions of sub-atomic particles which are deflected by the electromagnetic force. **Rutherford scattering**is the elastic scattering of charged particles also by the electromagnetic force.- A
**neutron-nucleus scattering reaction**may be also elastic, but in this case the neutron is deflected by the strong nuclear force.

**one dimensional elastic collision**of two objects, the object A and the object B. These two objects are moving with velocities

**v**and

_{A}**v**along the x axis before the collision. After the collision, their velocities are

_{B}**v’**and

_{A}**v’**. The

_{B}**conservation of the total momentum**demands that the total momentum before the collision is the same as the total momentum after the collision. Likewise, the

**conservation of the total kinetic energy**, which demands that the total kinetic energy of both objects before the collision is the same as the total kinetic energy after the collision. Both law may be expressed in equations as:

**The relative speed of the two objects** after the collision has **the same magnitude** (but opposite direction) as before the collision, **no matter what the masses are**.

It is known the fission neutrons are of importance in any chain-reacting system. All neutrons produced by fission are born as **fast neutrons** with high kinetic energy. Before such neutrons can efficiently cause additional fissions, they must be slowed down by collisions with nuclei in the moderator of the reactor. The probability of the fission U-235 becomes very large **at the thermal energies** of slow neutrons. This fact implies increase of multiplication factor of the reactor (i.e. lower fuel enrichment is needed to sustain chain reaction).

The neutrons released during fission with an average energy of **2 MeV** in a reactor on average undergo a **number of collisions** (elastic or inelastic) before they are absorbed. During the scattering reaction, a fraction of the neutron’s kinetic energy **is transferred to the nucleus**. Using the laws of **conservation of momentum and energy** and the analogy of collisions of billiard balls for elastic scattering, it is possible to derive the following equation for the mass of target or moderator nucleus (M), energy of incident neutron (E_{i}) and the energy of scattered neutron (E_{s}).

where A is the atomic mass number.In case of the **hydrogen (A = 1)** as the target nucleus, the incident neutron **can be completely stopped**. But this works when the direction of the neutron is completely reversed (i.e. scattered at 180°). In reality, the direction of scattering ranges from 0 to 180 ° and the energy transferred also ranges from 0% to maximum. Therefore, the average energy of scattered neutron is taken as the average of energies with scattering angle 0 and 180°.

Moreover, it is useful to work **with logarithmic quantities** and therefore one defines **the logarithmic energy decrement per collision (ξ)** as a key material constant describing energy transfers during a neutron slowing down. ξ is not dependent on energy, only on A and is defined as follows:For heavy target nuclei,** ξ** may be approximated by following formula:From these equations it is easy to determine the number of collisions required to slow down a neutron from, for example from **2 MeV to 1 eV**.

Example: Determine the number of collisions required for thermalization for the 2 MeV neutron in the carbon.

ξ_{CARBON} = 0.158

N(**2MeV → 1eV**) = ln 2⋅10^{6}/ξ =14.5/0.158 = **92**

For a mixture of isotopes:

**A neutron (n)**of mass

**1.01 u**traveling with a speed of

**3.60 x 10**interacts with a

^{4}m/s**carbon (C)**nucleus (

**m**) initially at rest in an

_{C}= 12.00 u**elastic head-on collision**.

What are the velocities of the neutron and carbon nucleus after the collision?

**Solution:**

This is an **elastic head-on collision** of two objects with **unequal masses**. We have to use the conservation laws of momentum and of kinetic energy, and apply them to our system of two particles.

We can solve this system of equation or we can use the equation derived in previous section. This equation stated that the relative speed of the two objects after the collision has the same magnitude (but opposite direction) as before the collision, no matter what the masses are.

The minus sign for v’ tells us that the **neutron scatters back** of the carbon nucleus, because the carbon nucleus is significantly heavier. On the other hand **its speed is less** than its initial speed. This process is known as the** neutron moderation** and it significantly depends on the mass of moderator nuclei.

## Inelastic Collisions

**An inelastic collision**is one in which part of the

**kinetic energy is changed**to some other form of energy in the collision. Any macroscopic collision between objects will convert some of the kinetic energy into

**internal energy**and other forms of energy, so

**no large scale impacts are perfectly elastic**. For example, in collisions of common bodies, such as two cars, some energy is always transferred from

**kinetic energy**to other forms of energy, such as

**thermal energy**or

**energy of sound**. The inelastic collision of two bodies always involves a loss in the kinetic energy of the system. The greatest loss occurs if the bodies stick together, in which case the collision is called a

**completely inelastic collision**. Thus, the

**kinetic energy**of the system is

**not conserved**, while the

**total energy is conserved**as required by the general principle of conservation of energy.

**Momentum is conserved in inelastic collisions**, but one cannot track the kinetic energy through the collision since some of it is converted to other forms of energy.

**In nuclear physics**, an inelastic collision is one in which the incoming particle causes the nucleus it strikes to become excited or to break up. Deep inelastic scattering is a method of probing the structure of subatomic particles in much the same way as Rutherford probed the inside of the atom (see Rutherford scattering).

**In nuclear reactors**, inelastic collisions are of importance in **neutron moderation** process. An inelastic scattering plays an important role in slowing down neutrons especially **at high energies and by heavy nuclei**. Inelastic scattering occurs above **a threshold energy**. This threshold energy is higher than the energy the first excited state of target nucleus (due to the laws of conservation) and it is given by following formula:

**E**_{t}** = ((A+1)/A)* ε**_{1}

where **E**** _{t}** is known as the

**inelastic threshold energy**and

**ε**

**is the energy of the first excited state. Therefore especially scattering data of**

_{1}

^{238}**U**, which is a major component of nuclear fuel in commercial power reactors, are one of the most important data in the neutron transport calculations in the reactor core.

**A ballistic pendulum** is a device for measuring the velocity of a projectile, such as a **bullet**. The ballistic pendulum is a kind of “transformer,” exchanging the high speed of a light object (the bullet) for the low speed of a massive object (the block). When a bullet is fired into the block, its momentum is transferred to the block. The bullet’s momentum can be determined from the** amplitude of the pendulum swing**.

When the bullet is embedding itself in the block, it occurs so quickly that the block does not move appreciably. The supporting strings remain nearly vertical, so negligible external horizontal force acts on the bullet–block system, and the** horizontal** component of **momentum is conserved**. **Mechanical energy is not conserved** during this stage, however, because a **nonconservative force** does work (the force of friction between bullet and block).

In the second stage, the bullet and block move together. The only forces acting on this system are gravity (a conservative force) and the string tensions (which do no work). Thus, as the block swings, **mechanical energy is conserved**. **Momentum is not conserved during this stage**, however, because there is a net external force (the forces of gravity and string tension don’t cancel when the strings are inclined).

**Equations governing the ballistic pendulum**

**Equations governing the ballistic pendulum**

In the first stage **momentum is conserved** and therefore:

where** v** is the initial velocity of the projectile of mass **m _{P}**.

**v’**is the velocity of the block and embedded projectile (both of mass

**m**) just after the collision, before they have moved significantly.

_{P}+ m_{B}In the second stage **mechanical energy is conserved**. We choose y = 0 when the pendulum hangs vertically, and then y = h when the block and embedded projectile system reaches its maximum height. The system swings up and comes to rest for an instant at a height y, where its kinetic energy is zero and the potential energy is **(m _{P} + m_{B})gh**. Thus we write the law of conservation of energy:

which is the initial velocity of the projectile and our final result.

**When we use some realistic numbers:**

- m
_{P}= 5 g - m
_{B}= 2 kg - h = 3 cm
- v = ?

**then we have:**

## Conservation of Energy in Fluid Mechanics – Bernoulli’s Principle

**flowing**

**fluids**.

**The Bernoulli’s equation** can be considered to be a statement of the **conservation of energy principle** appropriate for flowing fluids. It is one of the most important/useful equations in **fluid mechanics**. It puts into a relation **pressure and velocity** in an **inviscid incompressible flow**. The general energy equation is simplified to:

This equation is the most famous equation in **fluid dynamics**. **The Bernoulli’s equation** describes the qualitative behavior flowing fluid that is usually labeled with the term **Bernoulli’s effect**. This effect causes the **lowering of fluid pressure** in regions where the flow velocity is increased. This lowering of pressure in a constriction of a flow path may seem counterintuitive, but seems less so when you consider pressure to be** energy density**. In the high velocity flow through the constriction, **kinetic energy** must increase at the expense of **pressure energy**. The dimensions of terms in the equation are kinetic energy per unit volume. The equation above assumes that no **non-conservative forces** (e.g. friction forces) are acting on the fluid. This is very strong assumption.

**Extended Bernoulli’s equation**

The Bernoulli’s equation can be modified to take into account **gains and losses of head, **caused by **external forces** and **non-conservative forces**. The resulting equation, referred to as the **extended Bernoulli’s equation**, is very useful in solving most fluid flow problems. The following equation is one form of the extended Bernoulli’s equation.

where:

- h = height above reference level (m)
- v = average velocity of fluid (m/s)
- p = pressure of fluid (Pa)
- H
_{pump}= head added by pump (m) - H
_{friction}= head loss due to fluid friction (m) - g = acceleration due to gravity (m/s
^{2})

**The head loss** (or the pressure loss) due to fluid friction (H_{friction}) represents the energy used in overcoming friction caused by the walls of the pipe. The head loss that occurs in pipes is dependent on the **flow velocity, pipe diameter **and** length**, and a **friction factor** based on the roughness of the pipe and the **Reynolds number** of the flow. A piping system containing many pipe fittings and joints, tube convergence, divergence, turns, surface roughness and other physical properties will also increase the head loss of a hydraulic system.

Although the **head loss represents a loss of energy**, it does **does not represent a loss of total energy** of the fluid. The total energy of the fluid conserves as a consequence of the **law of conservation of energy**. In reality, the head loss due to friction results in an equivalent **increase in the internal energy** (increase in temperature) of the fluid.

This phenomenon can be seen also in case of reactor coolant pumps. Generally reactor coolant pumps are very powerful, they can consume **up to 6 MW each** and therefore they can be used for heating the primary coolant before a reactor startup. For example from 30°C at cold zero power (CZP) up to 290°C at hot zero power (HZP).

## Conservation of Energy in Thermodynamics – The First Law of Thermodynamics

**In thermodynamics**the concept of energy is broadened to account for other observed changes, and the

**principle of conservation of energy**is extended to include a wide variety of ways in which systems interact with their surroundings. The only ways the energy of a closed system can be changed are through transfer of energy

**by work**or

**by heat**. Further, based on the experiments of Joule and others, a fundamental aspect of the energy concept is that

**energy is conserved.**This principle is known as

**the first law of thermodynamics**. The first law of thermodynamics can be written in various forms:

**In words:**

**Equation form:**

**∆E**_{int}** = Q – W**

where **E _{int }**represents the

**internal energy**of the material, which depends only on the

**material’s state**(temperature, pressure, and volume).

**Q**is the

**net heat added**to the system and

**W**is the

**net work done by**the system. We must be careful and consistent in following the sign conventions for Q and W. Because W in the equation is the work done by the system, then if work is done on the system, W will be negative and E

_{int}will increase.

Similarly, Q is positive for heat added to the system, so if heat leaves the system, Q is negative. This tells us the following: The **internal energy** of a system tends to increase if heat is absorbed by the system or if positive work is done on the system. Conversely, the internal energy tends to decrease if heat is lost by the system or if negative work is done on the system. It must be added Q and W are path dependent, while E_{int} is path independent.

**Differential form:**

**dE _{int} = dQ – dW**

The internal energy E_{int} of a system tends to increase if energy is added as heat Q and tends to decrease if energy is lost as work W done by the system.

**Open System – Closed System – Isolated System**

**Heat and/or work** can be directed** into** or **out** of the **control volume**. But, for convenience and as a standard convention, the net energy exchange is presented here with the net heat exchange assumed to be into the system and the net work assumed to be out of the system. If **no mass crosses the boundary**, but work and/or heat do, then the system is referred to as a **“closed” system**. If mass, work and heat do not cross the boundary (that is, the only energy exchanges taking place are within the system), then the system is referred to as an** isolated system**. Isolated and closed systems are nothing more than specialized cases of the **open system**.

## Conservation of Energy in Electrical Circuits

### Kirchhoff’s voltage law (KVL)

**The law of conservation of energy** can be used also in the analysis of **electrical circuits**. In the analysis of electrical circuits the principle of energy conservation provides basis for the law, which is known as **Kirchhoff’s voltage law** (or **Kirchhoff’s second law**), after German physicist Gustav Robert Kirchhoff.

**Kirchhoff’s voltage law states:**

*The algebraic sum of the voltages (drops or rises) encountered in traversing any loop of a circuit in a specified direction must be zero.*

The algebraic sum of the voltages (drops or rises) encountered in traversing any loop of a circuit in a specified direction must be zero.

Simply, the voltage changes around any closed loop must sum to zero. The sum of the **voltage rises** is equal to the sum of the** voltage drops** in a loop. No matter what path you take through an electric circuit, if you return to your starting point you must measure the same voltage, constraining the net change around the loop to be zero.

Since **voltage** is **electric potential energy** per unit charge, the voltage law can be seen to be a consequence of **conservation of energy**. This rule is equivalent to saying that each point on a mountain has only one elevation above sea level. If you start from any point and return to it after walking around the mountain, the algebraic sum of the changes in elevation that you encounter must be zero.

The voltage law has great practical utility in the analysis of electric circuits. It is used in conjunction with the current law in many circuit analysis tasks.

## Conservation of Energy in Chemical Reactions

**chemistry.**Chemical reactions are determined by the

**laws of thermodynamics**. In thermodynamics, the

**internal energy**of a system is the energy contained within the system, excluding the kinetic energy of motion of the system as a whole and the potential energy of the system as a whole due to external force fields.

**In thermodynamics**, the **internal energy** include the **translational kinetic energy** of the molecules (in case of gases), the kinetic energy due to **rotation** of the molecules relative to their centers of mass and the kinetic energy associated with **vibrational motions** within the molecules.

**In chemical reactions**, energy is stored in the **chemical bonds** between the atoms that make up the molecules. **Energy storage** on the atomic level includes energy associated with electron orbital states. Whether a chemical reaction absorbs or releases energy, there is no overall change in the amount of energy during the reaction. That’s because of the** law of conservation of energy**, which states that:

**Energy cannot be created or destroyed**. **Energy may change form during a chemical reaction**.

For example, energy may change form from chemical energy to heat energy when gas burns in a furnace. The exact amount of energy remains after the reaction as before. This is true of all chemical reactions.

In an** endothermic reaction**, the products have more stored chemical energy than the reactants. In an **exothermic reaction**, the opposite is true. The products have less stored chemical energy than the reactants. The excess energy is generally released to the surroundings when the reaction occurs.

## Example: Combustion of Hydrogen

Consider the **combustion of hydrogen** in air. In a flame of pure hydrogen gas, burning in air, the **hydrogen (H _{2})** reacts with

**oxygen (O**to form

_{2})**water (H**and

_{2}O)**releases energy**.

Energetically, the process can be considered to require the energy to dissociate the **H _{2} **and

**O**, but then the bonding of the H

_{2}_{2}O returns the system to a bound state with

**negative potential**. It is actually

**more negative**than the bound states of the reactants, and the formation of the two water molecules is therefore an

**exothermic reaction**, which releases 5.7 eV of energy.

**2H _{2}(g) + O_{2}(g) → 2H_{2}O(g)**

The balance of energy before and after the reaction can be illustrated schematically with the state in which all atoms are free taken as the reference for energy.

## Law of Conservation of Mass-Energy – Mass-Energy Equivalence

**absoluteness**. One of the striking results of

**Einstein’s theory of relativity**is that

**mass and energy are equivalent and convertible**one into the other.

**Equivalence**of the mass and energy is described by Einstein’s famous formula

**E = mc**. In words,

^{2}**energy**equals

**mass**multiplied by the

**speed of light squared**. Because the speed of light is a very large number, the formula implies that any small amount of matter contains a very large amount of energy. The mass of an object was seen to be equivalent to energy, to be interconvertible with energy, and to increase significantly at exceedingly high speeds near that of light. The

**total energy**of an object was understood to comprise its

**rest mass**as well as its

**increase of mass**caused by

**increase in kinetic energy**.

**In special theory of relativity** certain types of **matter may be created or destroyed**, but in all of these processes, the mass and energy associated with such matter **remains unchanged in quantity**. It was found the **rest mass an atomic nucleus is measurably smaller than the sum of the rest masses of its constituent protons, neutrons and electrons**. Mass was no longer considered unchangeable in the closed system. The difference is a measure of the nuclear binding energy which holds the nucleus together. According to the Einstein relationship (**E = mc ^{2}**) this binding energy is proportional to this mass difference and it is known as the

**mass defect**.

**mass defect**of a

**nucleus if the actual mass of**

^{63}Cu^{63}Cu in its

**nuclear ground state is 62.91367 u.**

^{63}Cu nucleus has 29 protons and also has (63 – 29) 34 neutrons.

The mass of a proton is **1.00728 u** and a neutron is **1.00867 u**.

The combined mass is: 29 protons x (1.00728 u/proton) + 34 neutrons x (1.00867 u/neutron) = **63.50590 u**

**The mass defect** is Δm = 63.50590 u – 62.91367 u = **0.59223 u**

**Convert the mass defect into energy (nuclear binding energy).**

(0.59223 u/nucleus) x (1.6606 x 10^{-27} kg/u) = **9.8346 x 10 ^{-28} kg/nucleus**

ΔE = (9.8346 x 10^{-28} kg/nucleus) x (2.9979 x 10^{8} m/s)^{2} = **8.8387 x 10 ^{-11} J/nucleus**

The energy calculated in the previous example is the **nuclear binding energy**. However, the nuclear binding energy may be expressed as kJ/mol (for better understanding).

Calculate the nuclear binding energy of 1 mole of ^{63}Cu:

(8.8387 x 10^{-11} J/nucleus) x (1 kJ/1000 J) x (6.022 x 10^{23} nuclei/mol) = **5.3227 x 10 ^{10} kJ/mol of nuclei.**

One mole of ^{63}Cu (~63 grams) is bound by the nuclear binding energy (5.3227 x 10^{10} kJ/mol) which is equivalent to:

**14.8 million kilowatt-hours (≈ 15 GW·h)****336,100 US gallons of automotive gasoline**

**mass defect**of the

**3000MW**reactor core after one year of operation.

_{th}It is known the average recoverable energy per fission is about **200 MeV**, being the total energy minus the energy of the energy of antineutrinos that are radiated away.

The **reaction rate** per entire **3000MW _{th}** reactor core is about

**9.33×10**.

^{19}fissions / second**The overall energy release** in the units of joules is:

200×10^{6} (eV) x 1.602×10^{-19} (J/eV) x 9.33×10^{19} (s^{-1}) x 31.5×10^{6} (seconds in year) = **9.4×10 ^{16} J/year**

The mass defect is calculated as:

Δm = ΔE/c^{2}

**Δm** = 9.4×10^{16} / (2.9979 x 10^{8})^{2} = **1.046 kg**

That means in a typical **3000MWth** reactor core about 1 kilogram of matter is **converted** into pure energy.

Note that, a typical annual uranium load for a **3000MWth **reactor core is about **20 tonnes** of **enriched uranium **(i.e. about **22.7 tonnes of UO _{2}**). Entire reactor core may contain about 80 tonnes of enriched uranium.

### Mass defect directly from E=mc^{2}

The mass defect can be calculated directly from the Einstein relationship (**E = mc ^{2}**) as:

Δm = ΔE/c^{2}

Δm = 3000×10^{6} (W = J/s) x 31.5×10^{6} (seconds in year) / (2.9979 x 10^{8})^{2 }= **1.051 kg**

During the **nuclear splitting** or **nuclear fusion**, some of the mass of the nucleus gets converted into huge amounts of energy and thus this mass is removed from the total mass of the original particles, and the mass is missing in the resulting nucleus. **The nuclear binding energies** are enormous, they are of the order of a million times greater than the electron binding energies of atoms.

Generally, in both **chemical** and **nuclear reactions**, some conversion between rest mass and energy occurs, so that the products generally have smaller or greater mass than the reactants. Therefore the new conservation principle is **the conservation of mass-energy**.

See also: Energy Release from Fission

## Conservation Laws in Nuclear Reactions

**nuclear reaction**is considered to be the process in which two nuclear particles (two nuclei or a nucleus and a nucleon) interact to produce two or more nuclear particles or ˠ-rays (gamma rays). Thus, a

**nuclear reaction**must cause a transformation of at least one nuclide to another. Sometimes if a nucleus interacts with another nucleus or particle without changing the nature of any nuclide, the process is referred to a

**nuclear scattering**, rather than a nuclear reaction.

In analyzing nuclear reactions, we apply the **many conservation laws**. **Nuclear reactions** are subject to classical **conservation laws for charge, momentum, angular momentum, and energy** (including rest energies). Additional conservation laws, not anticipated by classical physics, are are **electric charge**, **lepton number and baryon number**. Certain of these laws are obeyed under all circumstances, others are not. We have accepted conservation of energy and momentum. In all the examples given we assume that the number of protons and the number of neutrons is separately conserved. We shall find circumstances and conditions in which this rule is not true. Where we are considering non-relativistic nuclear reactions, it is essentially true. However, where we are considering relativistic nuclear energies or those involving the weak interactions, we shall find that these principles must be extended.

Some conservation principles have arisen from theoretical considerations, others are just empirical relationships. Notwithstanding, any reaction not expressly forbidden by the conservation laws will generally occur, if perhaps at a slow rate. This expectation is based on quantum mechanics. Unless the barrier between the initial and final states is infinitely high, there is always a **non-zero probability** that a system will make the transition between them.

For purposes of this article it is sufficient to note four of the fundamental laws governing these reactions.

**Conservation of nucleons**. The total number of nucleons before and after a reaction are the same.**Conservation of charge**. The sum of the charges on all the particles before and after a reaction are the same**Conservation of momentum**. The total momentum of the interacting particles before and after a reaction are the same.**Conservation of energy**. Energy, including rest mass energy, is conserved in nuclear reactions.

**nuclear reactions**is enormous, nuclear reactions can be sorted by types. Most of nuclear reactions are accompanied by gamma emission. Some examples are:

**Elastic scattering**. Occurs, when no energy is transferred between the target nucleus and the incident particle.

** 208Pb (n, n) 208Pb**

**Inelastic scattering**. Occurs, when energy is transferred. The difference of kinetic energies is saved in excited nuclide.

** 40Ca (α, α’) 40mCa**

**Capture reactions**. Both charged and neutral particles can be captured by nuclei. This is accompanied by the emission of ˠ-rays. Neutron capture reaction produces radioactive nuclides (induced radioactivity).

** 238U (n, ˠ) 239U**

**Transfer Reactions**. The absorption of a particle accompanied by the emission of one or more particles is called the transfer reaction.

**4He (α, p) 7Li**

**Fission reactions**. Nuclear fission is a nuclear reaction in which the nucleus of an atom splits into smaller parts (lighter nuclei). The fission process often produces free neutronsand photons (in the form of gamma rays), and releases a large amount of energy.

**235U (n, 3 n) fission products**

**Fusion reactions**. Occur when, two or more atomic nuclei collide at a very high speed and join to form a new type of atomic nucleus.The fusion reaction of deuterium and tritium is particularly interesting because of its potential of providing energy for the future.

**3T (d, n) 4He**

**Spallation reactions**. Occur, when a nucleus is hit by a particle with sufficient energy and momentum to knock out several small fragments or, smash it into many fragments.

**Nuclear decay**(**Radioactive decay**). Occurs when an unstable atom loses energy by emitting ionizing radiation. Radioactive decay is a random process at the level of single atoms, in that, according to quantum theory, it is impossible to predict when a particular atom will decay. There are many types of radioactive decay:**Alpha radioactivity**. Alpha particles consist of two protons and two neutrons bound together into a particle identical to a helium nucleus. Because of its very large mass (more than 7000 times the mass of the beta particle) and its charge, it heavy ionizes material and has a very short range.

**Beta radioactivity**. Beta particles are high-energy, high-speed electrons or positrons emitted by certain types of radioactive nuclei such as potassium-40. The beta particles have greater range of penetration than alpha particles, but still much less than gamma rays.The beta particles emitted are a form of ionizing radiation also known as beta rays. The production of beta particles is termed beta decay.

**Gamma radioactivity**. Gamma rays are electromagnetic radiation of an very high frequency and are therefore high energy photons. They are produced by the decay of nuclei as they transition from a high energy state to a lower state known as gamma decay. Most of nuclear reactions are accompanied by gamma emission.

**Neutron emission.**Neutron emission is a type of radioactive decay of nuclei containing excess neutrons (especially fission products), in which a neutron is simply ejected from the nucleus. This type of radiation plays key role in nuclear reactor control, because these neutrons are delayed neutrons.

## Conservation of Energy in Nuclear Reactions

**mass and energy are equivalent and convertible**one into the other. It is one of the striking results of

**Einstein’s theory of relativity**. This

**equivalence**of the mass and energy is described by Einstein’s famous formula

**E = mc**

**.**

^{2}Generally, in both **chemical** and **nuclear reactions**, some conversion between rest mass and energy occurs, so that the products generally have smaller or greater mass than the reactants. In general, the total (relativistic) energy must be conserved. The “missing” rest mass must therefore reappear as kinetic energy released in the reaction. The difference is a measure of the nuclear binding energy which holds the nucleus together.

**The nuclear binding energies** are enormous, they are of the order of a million times greater than the electron binding energies of atoms.

The **energetics of nuclear reactions** is determined by the **Q-value** of that reaction. The **Q-value** of the reaction is defined as the **difference** between the sum of the **masses** of the **initial reactants** and the sum of the **masses** of the **final products**, in energy units (usually in MeV).

Consider a typical reaction, in which the projectile a and the target A gives place to two products, B and b. This can also be expressed in the notation that we used so far, **a + A → B + b**, or even in a more compact notation, **A(a,b)B**.

See also: E=mc^{2}

The **Q-value** of this reaction is given by:

**Q = [m**_{a}** + m**_{A}** – (m**_{b}** + m**_{B}**)]c**^{2}

which is the same as the **excess kinetic energy** of the final products:

**Q = T**_{final}** – T**_{initial}

** = T**_{b}** + T**_{B}** – (T**_{a}** + T**_{A}**)**

For reactions in which there is an increase in the kinetic energy of the products **Q is positive**. The positive Q reactions are said to be **exothermic** (or **exergic**). There is a net release of energy, since the kinetic energy of the final state is greater than the kinetic energy of the initial state.

For reactions in which there is a decrease in the kinetic energy of the products **Q is negative**. The negative Q reactions are said to be **endothermic** (or **endoergic**) and they require a net energy input.

See also: Q-value Calculator

**The DT fusion reaction** of deuterium and tritium is particularly interesting because of its potential of providing energy for the future. Calculate the reaction **Q-value**.

**3T (d, n) 4He**

The atom masses of the reactants and products are:

m(^{3}T) = 3.0160 amu

m(^{2}D) = 2.0141 amu

m(^{1}n) = 1.0087 amu

m(^{4}He) = 4.0026 amu

Using the mass-energy equivalence, we get the **Q-value** of this reaction as:

Q = {(3.0160+2.0141) [amu] – (1.0087+4.0026) [amu]} x 931.481 [MeV/amu]

= 0.0188 x 931.481 = **17.5 MeV**

**reactor kinetics**and in

**a subcriticality control**. Especially in nuclear reactors with D

_{2}O moderator (CANDU reactors) or with Be reflectors (some experimental reactors). Neutrons can be produced also in

**(γ, n) reactions**and therefore they are usually referred to as

**photoneutrons**.

A high energy photon (gamma ray) can under certain conditions **eject** a neutron from a nucleus. It occurs when **its energy exceeds** the binding energy of the neutron in the nucleus. Most nuclei have binding energies in excess of **6 MeV**, which is above the energy of most gamma rays from fission. On the other hand **there are few nuclei** with sufficiently low binding energy to be of **practical interest**. These are: ** ^{2}D, ^{9}Be**,

^{6}Li,

^{7}Li and

^{13}C. As can be seen from the table

**the lowest threshold**have

**and**

^{9}Be with 1.666 MeV**.**

^{2}D with 2.226 MeVIn case of deuterium, neutrons can be produced by the interaction of gamma rays (with a minimum energy of 2.22 MeV) with deuterium:

The** reaction Q-value** is calculated below:

The atom masses of the reactant and products are:

m(^{2}D) = 2.01363 amu

m(^{1}n) = 1.00866 amu

m(^{1}H) = 1.00728 amu

Using the mass-energy equivalence, we get the Q-value of this reaction as:

Q = {2.01363 [amu] – (1.00866+1.00728) [amu]} x 931.481 [MeV/amu]

= -0.00231 x 931.481 = -2.15 MeV

**energy released in a nuclear reaction**can appear mainly in one of three ways:

**Kinetic energy**of the products**Emission of gamma rays**.**Gamma rays**are emitted by unstable nuclei in their transition from a high energy state to a lower state known as gamma decay.**Metastable state**. Some energy may remain in the nucleus, as a metastable energy level.

A small amount of energy may also emerge in the form of X-rays. Generally, products of nuclear reactions may have different atomic numbers, and thus the configuration of their electron shells is different in comparison with reactants. As the **electrons rearrange** themselves and drop to lower energy levels, internal transition X-rays (X-rays with precisely defined emission lines) may be emitted.

## Energy Conservation in Nuclear Fission

**nuclear fission**results in the release of

**enormous quantities of energy**. The amount of energy

**depends strongly on**the nucleus to be fissioned and also depends strongly on the kinetic energy of an incident neutron. In order to calculate the power of a reactor, it is necessary to be able precisely identify the

**individual components of this energy**. At first, it is important to distinguish between

**the total energy released**and

**the energy that can be recovered in a**

**reactor**.

**The total energy released** in fission can be calculated from binding energies of initial target nucleus to be fissioned and binding energies of fission products. But not all the total energy can be recovered in a reactor. For example, **about 10 MeV** is released in the form of neutrinos (in fact antineutrinos). Since the neutrinos are weakly interacting (with extremely low cross-section of any interaction), they do not contribute to the energy that can be recovered in a reactor.

See also: Energy Release from Fission

**mass defect**of the

**3000MW**reactor core after one year of operation.

_{th}It is known the average recoverable energy per fission is about **200 MeV**, being the total energy minus the energy of the energy of antineutrinos that are radiated away.

The **reaction rate** per entire **3000MW _{th}** reactor core is about

**9.33×10**.

^{19}fissions / second**The overall energy release** in the units of joules is:

200×10^{6} (eV) x 1.602×10^{-19} (J/eV) x 9.33×10^{19} (s^{-1}) x 31.5×10^{6} (seconds in year) = **9.4×10 ^{16} J/year**

The mass defect is calculated as:

Δm = ΔE/c^{2}

**Δm** = 9.4×10^{16} / (2.9979 x 10^{8})^{2} = **1.046 kg**

That means in a typical **3000MWth** reactor core about 1 kilogram of matter is **converted** into pure energy.

Note that, a typical annual uranium load for a **3000MWth **reactor core is about **20 tonnes** of **enriched uranium **(i.e. about **22.7 tonnes of UO _{2}**). Entire reactor core may contain about 80 tonnes of enriched uranium.

### Mass defect directly from E=mc^{2}

The mass defect can be calculated directly from the Einstein relationship (**E = mc ^{2}**) as:

Δm = ΔE/c^{2}

Δm = 3000×10^{6} (W = J/s) x 31.5×10^{6} (seconds in year) / (2.9979 x 10^{8})^{2 }= **1,051 kg**

## Energy Conservation in Beta Decay – Discovery of the Neutrino

**Beta decay**(β-decay) is a type of radioactive decay in which a beta particle, and a respective neutrino are emitted from an atomic nucleus.

**Beta radiation**consist of

**beta particles**that are high-energy, high-speed

**electrons or positrons**are emitted during beta decay. By beta decay emission, a neutron is transformed into a proton by the emission of an electron, or conversely a proton is converted into a neutron by emission of a positron, thus changing the nuclide type.

### Discovery of the Neutrino

The study of beta decay provided the first physical evidence for the **existence of the neutrino**. The **discovery of the neutrino** is based on the **law of conservation of energy** during the process of beta decay.

In both alpha and gamma decay, the resulting particle (alpha particle or photon) has a **narrow energy distribution**, since the particle carries the energy from the difference between the initial and final nuclear states. For example, in case of alpha decay, when a parent nucleus breaks down spontaneously to yield a daughter nucleus and an alpha particle, the sum of the mass of the two products does not quite equal the mass of the original nucleus (see Mass Defect). As a result of the law of conservation of energy, this difference appears in the form of the** kinetic energy of the alpha particle**. Since the same particles appear as products at every breakdown of a particular parent nucleus, the mass-difference should **always be the same**, and the** kinetic energy** of the alpha particles should also always be the same. In other words, the beam of alpha particles should be **monoenergetic**.

It was expected that the same considerations would hold for a parent nucleus breaking down to a daughter nucleus and **a beta particle**. Because only the electron and the recoiling daughter nucleus were observed beta decay, the process was initially **assumed to be a two body process**, very much like alpha decay. It would seem reasonable to suppose that the beta particles would form also a **monoenergetic beam**.

To demonstrate energetics of two-body beta decay, consider the beta decay in which an electron is emitted and the parent nucleus is at rest, **conservation of energy** requires:

Since the electron is much lighter particle it was expected that it will carry away most of the released energy, which would have a unique value **T**** _{e-}**.

**But the reality was different**. The spectrum of beta particles measured by Lise Meitner and Otto Hahn in 1911 and by Jean Danysz in 1913 showed multiple lines on a diffuse background, however. Moreover virtually all of the emitted beta particles have energies below that predicted by energy conservation in two-body decays. **The electrons emitted in beta decay have a continuous rather than a discrete spectrum** appeared to contradict conservation of energy, under the then-current assumption that beta decay is the simple emission of an electron from a nucleus. When this was first observed, **it appeared to threaten the survival of one of the most important conservation laws in physics**!

To account for this energy release, **Pauli proposed** (in 1931) that there was emitted in the decay process **another particle**, later named by Fermi the** neutrino**. It was clear, this particle must be highly penetrating and that the conservation of electric charge requires the neutrino to be electrically neutral. This would explain why it was so hard to detect this particle. The term neutrino comes from Italian meaning “little neutral one” and neutrinos are denoted by the Greek letter** ν (nu)**. In the process of beta decay the neutrino carries the missing energy and also in this process the law of **conservation of energy remains valid**.

**Nuclear and Reactor Physics:**

- J. R. Lamarsh, Introduction to Nuclear Reactor Theory, 2nd ed., Addison-Wesley, Reading, MA (1983).
- J. R. Lamarsh, A. J. Baratta, Introduction to Nuclear Engineering, 3d ed., Prentice-Hall, 2001, ISBN: 0-201-82498-1.
- W. M. Stacey, Nuclear Reactor Physics, John Wiley & Sons, 2001, ISBN: 0- 471-39127-1.
- Glasstone, Sesonske. Nuclear Reactor Engineering: Reactor Systems Engineering, Springer; 4th edition, 1994, ISBN: 978-0412985317
- W.S.C. Williams. Nuclear and Particle Physics. Clarendon Press; 1 edition, 1991, ISBN: 978-0198520467
- Kenneth S. Krane. Introductory Nuclear Physics, 3rd Edition, Wiley, 1987, ISBN 978-0471805533
- G.R.Keepin. Physics of Nuclear Kinetics. Addison-Wesley Pub. Co; 1st edition, 1965
- Robert Reed Burn, Introduction to Nuclear Reactor Operation, 1988.
- U.S. Department of Energy, Nuclear Physics and Reactor Theory. DOE Fundamentals Handbook, Volume 1 and 2. January 1993.

**Advanced Reactor Physics:**

- K. O. Ott, W. A. Bezella, Introductory Nuclear Reactor Statics, American Nuclear Society, Revised edition (1989), 1989, ISBN: 0-894-48033-2.
- K. O. Ott, R. J. Neuhold, Introductory Nuclear Reactor Dynamics, American Nuclear Society, 1985, ISBN: 0-894-48029-4.
- D. L. Hetrick, Dynamics of Nuclear Reactors, American Nuclear Society, 1993, ISBN: 0-894-48453-2.
- E. E. Lewis, W. F. Miller, Computational Methods of Neutron Transport, American Nuclear Society, 1993, ISBN: 0-894-48452-4.