Module 01 Energy Basics Energy Power Forms of energy Thermodynamic laws Entropy Exergy Combustion fundamentals Prof. R. Shanthini Dec 10, 2011 1 A few suggested references Shanthini, R., 2009. Thermodynamics for beginners. Peradeniya: Science Education Unit. Certain chapters available from: http://www.rshanthini.com/ThermoBook.htm MacKay, D.J.C., 2009. Sustainable energy: without the hot air. Cambridge: UIT Cambridge Ltd. Available from: http://www.withouthotair.com/download.html Prof. R. Shanthini Dec 10, 2011 2 • What is energy? – energy is the ability to do work (defined loosely) Energy is not a ‘thing’ or ‘substance’. Energy cannot be seen, heard or felt. Energy is a concept. Prof. R. Shanthini Dec 10, 2011 3 • What is energy? – energy is the ability to do work (defined loosely) • What is work? – force exerted over a distance (scientific definition) F F is the force pushing the ball Prof. R. Shanthini Dec 10, 2011 4 • What is energy? – energy is the ability to do work (defined loosely) • What is work? – force exerted over a distance (scientific definition) F F is the force pushing the ball D D is the distance over which the ball is moved Work = F x D Prof. R. Shanthini Dec 10, 2011 5 • What is energy? – energy is the ability to do work (defined loosely) Work = Force x Distance • What is power? – power is the rate at which work is done Power = Work / Time Prof. R. Shanthini Dec 10, 2011 6 • What is the unit of Energy? • What is the unit of Work? • What is the unit of Power? Prof. R. Shanthini Dec 10, 2011 7 Units for energy / work joule 1 J (joule) in SI-system = 1 N·m = 1 (N/m2) ·m3 = 1 Pa·m3 1 N (newton) = 1 (kg.m/s2) is the unit of force 1 Pa (pascal) = 1 N/m2 is the unit for pressure Prof. R. Shanthini Dec 10, 2011 8 SI multiples for joules (W) Submultiples Multiples Value Symbol Name Value Symbol Name 10−1 J dJ decijoule 101 J daJ decajoule 10−2 J cJ centijoule 102 J hJ hectojoule 10−3 J mJ millijoule 103 J kJ kilojoule 10−6 J µJ microjoule 106 J MJ megajoule 10−9 J nJ nanojoule 109 J GJ gigajoule 10−12 J pJ picojoule 1012 J TJ terajoule 10−15 J fJ femtojoule 1015 J PJ petajoule 10−18 J aJ attojoule 1018 J EJ exajoule 10−21 J zJ zeptojoule 1021 J ZJ zettajoule 10−24 J yJ yoctojoule 1024 J YJ yottajoule Prof. R. Shanthini Dec 10, 2011 9 http://en.wikipedia.org/wiki/Orders_of_magnitude_(energy) Units for power watt 1 W (watt) in SI-system = 1 J/s = 1 N.m/s 60 W = 60 J/s = 60*60 J/m = 60*60*60 J/h = 216,000 J/h = 216 kJ/h Prof. R. Shanthini Dec 10, 2011 10 SI multiples for watts (J) Submultiples Multiples Value Symbol Name Value Symbol Name 10−1 W dW deciwatt 101 W daW decawatt 10−2 W cW centiwatt 102 W hW hectowatt 10−3 W mW milliwatt 103 W kW kilowatt 10−6 W µW microwatt 106 W MW megawatt 10−9 W nW nanowatt 109 W GW gigawatt 10−12 W pW picowatt 1012 W TW terawatt 10−15 W fW femtowatt 1015 W PW petawatt 10−18 W aW attowatt 1018 W EW exawatt 10−21 W zW zeptowatt 1021 W ZW zettawatt 10−24 W yW yoctowatt 1024 W YW yottawatt Prof. R. Shanthini Dec 10, 2011 11 Global Energy Consumption Global Consumption = 15 TW = 15x1012 W = 250,000,000,000 of 60 W bulbs = about 35 of 60 W bulbs per person Prof. R. Shanthini Dec 10, 2011 12 http://en.wikipedia.org/wiki/Orders_of_magnitude_(energy) Global Energy Consumption Global Consumption = 15 TW = 15x1012 W = 250,000,000,000 of 60 W bulbs = about 35 of 60 W bulbs per person Prof. R. Shanthini Dec 10, 2011 13 http://en.wikipedia.org/wiki/Orders_of_magnitude_(energy) Global Energy Consumption Global Consumption = 15 TW = 15x1012 J/s = 54x1015 J/h Prof. R. Shanthini Dec 10, 2011 14 http://en.wikipedia.org/wiki/Orders_of_magnitude_(energy) One joule in everyday life is approximately: The energy required to raise the temperature of cool, dry air by one degree Celsius. A person at rest releases 100 joules of heat every second. Prof. R. Shanthini Dec 10, 2011 15 • What is energy? – energy is the ability to do work (defined loosely) • What is work? – force exerted over a distance (scientific definition) • Is heat energy too? – heat is a form of energy that flows from a warmer object to a cooler object – work sometimes gets converted to heat (think of examples) – heat sometimes gets converted to work (think of examples) Prof. R. Shanthini Dec 10, 2011 16 Units for heat Joule / Calorie 1 calorie = the energy needed to raise the temperature of 1 gram of water by 1oC = 4.184 J (joules) = 0.003 964 BTU (British thermal units) Prof. R. Shanthini Dec 10, 2011 17 For more on energy units and conversions, Visit The American Physical Society Site http://www.aps.org/policy/reports/popa-reports/energy/units.cfm Prof. R. Shanthini Dec 10, 2011 18 Basic Forms of Energy • • • • • • • • • Kinetic Energy: Potential Energy: Thermal (or Heat) Energy: Chemical Energy: Electrical Energy: Electrochemical Energy: Sound Energy: Electromagnetic Energy (light): Nuclear Energy: Prof. R. Shanthini Dec 10, 2011 19 Basic Forms of Energy (continued) • Thermal (or Heat) Energy: – Consider a hot cup of coffee. The coffee is said to possess "thermal energy", or "heat energy," which is really the collective, microscopic, kinetic, and potential energy of the molecules in the coffee. • Chemical Energy: – Consider the ability of your body to do work. The glucose (blood sugar) in your body is said to have "chemical energy" because the glucose releases energy when chemically reacted (combusted) with oxygen. Prof. R. Shanthini Dec 10, 2011 20 Source: http://euclidstube.com/poe/Thermodynamics.ppt Basic Forms of Energy (continued) • Electrical Energy: – All matter is made up of atoms, and atoms are made up of smaller particles, called protons, neutrons, and electrons. Electrons orbit around the center, or nucleus, of atoms, just like the moon orbits the earth. The nucleus is made up of neutrons and protons. – Material, like metals, have certain electrons that are only loosely attached to their atoms. They can easily be made to move from one atom to another if an electric field is applied to them. When those electrons move among the atoms of matter, a current of electricity is created. Prof. R. Shanthini Dec 10, 2011 21 Source: http://euclidstube.com/poe/Thermodynamics.ppt Basic Forms of Energy (continued) • Electrochemical Energy: – Consider the energy stored in a battery. Like the example above involving blood sugar, the battery also stores energy in a chemical way. But electricity is also involved, so we say that the battery stores energy "electro-chemically". Another electron chemical device is a "fuel-cell". Prof. R. Shanthini Dec 10, 2011 22 Source: http://euclidstube.com/poe/Thermodynamics.ppt Basic Forms of Energy (continued) • Sound Energy: – Sound waves are compression waves associated with the potential and kinetic energy of air molecules. When an object moves quickly, for example the head of drum, it compresses the air nearby, giving that air potential energy. That air then expands, transforming the potential energy into kinetic energy (moving air). The moving air then pushes on and compresses other air, and so on down the chain. Prof. R. Shanthini Dec 10, 2011 23 Source: http://euclidstube.com/poe/Thermodynamics.ppt Basic Forms of Energy (continued) • Electromagnetic Energy (light): – Consider the energy transmitted to the Earth from the Sun by light (or by any source of light). Light, which is also called "electro-magnetic radiation". Why the fancy term? Because light really can be thought of as oscillating, coupled electric and magnetic fields that travel freely through space (without there having to be charged particles of some kind around). – It turns out that light may also be thought of as little packets of energy called photons (that is, as particles, instead of waves). The word "photon" derives from the word "photo", which means "light". Prof. R. Shanthini Dec 10, 2011 24 Source: http://euclidstube.com/poe/Thermodynamics.ppt Basic Forms of Energy (continued) • Nuclear Energy: – The Sun, nuclear reactors, and the interior of the Earth, all have "nuclear reactions" as the source of their energy, that is, reactions that involve changes in the structure of the nuclei of atoms. Prof. R. Shanthini Dec 10, 2011 25 Source: http://euclidstube.com/poe/Thermodynamics.ppt Energy is available in different forms. Energy cannot be created or destroyed (which is a natural law). Energy can change from one form to the other. Prof. R. Shanthini Dec 10, 2011 26 The study of conversion of energy is known as Thermodynamics. Mostly, it is study of the connection between heat and work, and the conversion of one into the other. Engineering examples: …………………………………… Prof. R. Shanthini Dec 10, 2011 27 Thermodynamics is based on fundamentals laws, which are the natural laws. These laws have not been proven wrong so far. These laws will remain as fundamental laws until someone finds out that they are wrong. If that happens then we need to redo all thermodynamics that has been developed so far. Prof. R. Shanthini Dec 10, 2011 28 First Law of Thermodynamics Energy is conserved. That means, energy cannot be created or destroyed. However, energy can change from one form to the other. Prof. R. Shanthini Dec 10, 2011 29 First Law of Thermodynamics System Energy of the system Qin E Wout Heat energy that entered the system Work energy that left the system Prof. R. Shanthini Dec 10, 2011 30 First Law of Thermodynamics Qin E Wout Efinal - Einitial = Qin – Wout Prof. R. Shanthini Dec 10, 2011 ΔE = Qin – Wout 31 First Law of Thermodynamics First law is about the balance of quantities of energy. It helps to keep account of what happen to all forms of energy that are involved in a process. Prof. R. Shanthini Dec 10, 2011 32 Apply First law to Heat Engine Hot reservoir at TH K Qin Heat Engine Wout A heat engine is a mechanical system. As it cycles through a repetitive motion, transfers heat from a high temperature heat bath to a low temperature bath, and performs work on its environment. Qout Cold reservoir at TC K Prof. R. Shanthini Dec 10, 2011 Example: Diesel cycle auto.howstuffworks.com/diesel.htm 33 Apply First law to Heat Engine Hot reservoir at TH K Qin Heat Engine First law gives the following relationship: Qin = Wout + Qout Wout Qout Cold reservoir at TC K Prof. R. Shanthini Dec 10, 2011 34 Hot reservoir at TH K Qin Heat Engine Wout We like to have an engine that converts all heat into work. That is, we would like to have Qin = Wout Is it possible? Prof. R. Shanthini Dec 10, 2011 35 Second Law of Thermodynamics Hot reservoir at TH K Qin Heat Engine Wout Qout Prof. R. Shanthini Dec 10, 2011 WHY? Second law of thermodynamics says it is not possible to convert all heat into work in an engine. It says it is necessary to throw away some heat to the environment. 36 Second Law of Thermodynamics Hot reservoir at TH K Qin Heat Engine Wout Qout Cold reservoir at TC K Prof. R. Shanthini Dec 10, 2011 Maximum possible thermal efficiency of the heat engine is η = 1 Carnot - TC TH Since TC can never be zero, η Carnot <1 37 Second Law of Thermodynamics Hot reservoir at TH K Qin Heat Engine Wout Qout Thermal efficiency of the heat engine is W out ηth = Qin ηth < η < 1 Carnot Cold reservoir at TC K Prof. R. Shanthini Dec 10, 2011 38 Second Law of Thermodynamics Hot reservoir at TH K Qin Heat Engine Wout Qout Cold reservoir at TC K Prof. R. Shanthini Dec 10, 2011 Thermal efficiency of the heat engine is W out ηth = Qin <1 Qin ≠ Wout Qout ≠ 0 39 Some heat is thrown away. Entropy When heat is transformed into work, as in the heat engines, some heat is always lost to the environment (according to the Second Law). This irrevocable loss of some energy to the environment is associated with an increase of disorder in that system. Entropy acts as a function of the state of a system - where a high amount of entropy translates to higher chaos within the system, and low entropy signals a highly ordered state. The Second Law tells that the quality of energy is degraded every time energy is used in any process. This ‘energy quality’ has been named exergy. Prof. R. Shanthini Dec 10, 2011 40 Exergy The Second Law tells us that the quality of a particular amount of energy diminishes for each time this energy is used. This means that the quality of energy in the universe as a whole is constantly diminishing. All real processes are irreversible, since the quality of the energy driving them is lowered for all times. Prof. R. Shanthini Dec 10, 2011 41 Exergy The Second Law tells us about the direction of the universe and all processes, namely towards a decreasing exergy content of the universe. Processes that follow this general principle will be preferred. The usable energy in a system is called exergy, and can be measured as the total of the free energies in the system. Unlike energy, exergy can be consumed. Prof. R. Shanthini Dec 10, 2011 42 The energy of the universe is constant (First Law). Exergy is constantly consumed (Second Law). In the end (very long time from now), exergy is used up in the universe, and no processes can run. The entropy of a system increases whenever exergy is lost. Prof. R. Shanthini Dec 10, 2011 43 Zeroth Law of Thermodynamics If object A is in thermal equilibrium with object C, and object B is in thermal equilibrium with object C, then object A & B are also in thermal equilibrium. Thermal Equilibrium = Same temperature Thermal Equilibrium = No heat flow Prof. R. Shanthini Dec 10, 2011 44 Third Law of Thermodynamics It is impossible to reach absolute zero in a finite number of steps. Prof. R. Shanthini Dec 10, 2011 45 Combustion Fundamentals Combustion is a process in which oxidizable materials such as fossil fuels are oxidized by use of oxygen (present in the air). During this process energy is released in the form of heat. Major combustion product is the global pollutant, carbon dioxide (CO2), which is a greenhouse gases. Combustion products also include other local pollutants. Combustion fundamentals include the nature of the fuels being burned, the nature of the products formed and the stoichiometry of the combustion reaction. Prof. R. Shanthini Dec 10, 2011 46 Combustion (or Fire) Triangle Prof. R. Shanthini Dec 10, 2011 47 Combustion Engine The combustion engine is used to power nearly all land vehicles and many water-based and air-based vehicles. In an internal combustion engine, a fuel (gasoline for example) fills a chamber, then it is compressed to heat it up, and then is ignited by a spark plug, causing a small explosion which generates work. Prof. R. Shanthini Dec 10, 2011 48 Combustion Engine Prof. R. Shanthini Dec 10, 2011 49 Combustion Engine Prof. R. Shanthini Dec 10, 2011 50 Combustion Engine Prof. R. Shanthini Dec 10, 2011 51 http://bancroft.berkeley.edu/Exhibits/physics/images/origins18.jpg Combustion Engine Prof. R. Shanthini Dec 10, 2011 52 http://images.yourdictionary.com/images/main/A4gastrb.jpg Combustion Fundamentals Stoichiometric (or theoretical) combustion is the ideal combustion process where fuel is burned completely. A complete combustion is a process burning - all the carbon (C) to (CO2), - all the hydrogen (H) to (H2O) and - all the sulphur (S) to (SO2). With unburned components in the exhaust gas, such as C, H2, CO, the combustion process is incomplete and not stoichiometric. Prof. R. Shanthini Dec 10, 2011 53 http://www.engineeringtoolbox.com/stoichiometric-combustion-d_399.html Combustion Fundamentals If an insufficient amount of air is supplied to the burner, unburned fuel, soot, smoke, and carbon monoxide exhausts from the boiler - resulting in heat transfer surface fouling, pollution, lower combustion efficiency, flame instability and a potential for explosion. To avoid inefficient and unsafe conditions boilers normally operate at an excess air level. Prof. R. Shanthini Dec 10, 2011 54 http://www.engineeringtoolbox.com/stoichiometric-combustion-d_399.html Combustion Fundamentals if air content is higher than the stoichiometric ratio - the mixture is said to be fuel-lean if air content is less than the stoichiometric ratio - the mixture is fuel-rich Prof. R. Shanthini Dec 10, 2011 55 http://www.engineeringtoolbox.com/stoichiometric-combustion-d_399.html Combustion Fundamentals Example - Stoichiometric Combustion of Methane - CH4 CH4 + 2 (O2 + 3.76 N2) -> CO2 + 2 H2O + 7.52 N2 If more air is supplied some of the air will not be involved in the reaction. The additional air is termed excess air, but the term theoretical air may also be used. 200% theoretical air is 100% excess air. The chemical equation for methane burned with 25% excess air can be expressed as CH4 + 1.25 x 2 (O2 + 3.76 N2) -> CO2 + 2 H2O + 0.5 O2 + 9.4 N2 Prof. R. Shanthini Dec 10, 2011 56 http://www.engineeringtoolbox.com/stoichiometric-combustion-d_399.html Combustion Fundamentals Excess Air and O2 and CO2 in Flue Gas Approximate values for CO2 and O2 in the flue gas as result of excess air (for various fuels) are estimated in the table below: Carbon Dioxide - CO2 - in Flue Gas (% volume) Oxygen in Flue Gas Bituminou Anthracite for all fuels (% s Coal Coal volume) Excess Air % Natural Gas Propane Butane Fuel Oil 0 12 14 15.5 18 20 0 20 10.5 12 13.5 15.5 16.5 3 40 9 10 12 13.5 14 5 60 8 9 10 12 12.5 7.5 80 7 8 9 11 11.5 9 100 6 6 8 9.5 10 10 Prof. R. Shanthini Dec 10, 2011 57 http://www.engineeringtoolbox.com/stoichiometric-combustion-d_399.html