COMBUSTION ENGINEERING By: Engr. YURI G. MELLIZA Fuel - a substance composed of chemical elements, which in rapid chemical union with oxygen produced combustion. Combustion - is that rapid chemical union with oxygen of an element, whose exothermic heat of reaction is sufficiently great and whose rate of reaction is sufficiently fast, whereby useful quantities of heat are liberated at elevated temperatures. It is the burning or oxidation of the combustible elements. TYPES OF FUEL 1) Solid Fuels Example: a. coal b. charcoal c. coke d. woods 2) Liquid Fuels (obtained by the distillation of petroleum) Example: a. Gasoline b. kerosene c. diesoline d. Fuel oil e. alcohol (these are not true hydrocarbons, since it contains oxygen in the molecule) 3) Gaseous Fuels (a mixture of various constituent’s hydrocarbons, its combustion products do not have sulfur components) Example: a. Natural Gas (example: methane, ethane, propane) b. Coke oven gas -obtained as a byproduct of making coke c. Blast furnace gas - a byproduct of melting iron ore d. LPG e. Producer Gas - fuel used for gas engines 4) Nuclear Fuels Example: a. Uranium b. Plutonium COMBUSTIBLE ELEMENTS 1. Carbon (C) 2. Hydrogen (H2) 3. Sulfur (S) TYPES OF HYDROCARBONS 1) Paraffin - all ends in "ane" Formula: CnH2n+2 Structure: Chain (saturated) Example: GAS a. Methane(CH4) b. Ethane (C2H6) LPG a. Propane (C3H8) b. Butane (C4H10) c. Pentane (C5H12) GASOLINE a. n-Heptane (C7H16) b. Triptane (C7H16) c. Iso- octane (C8H18) FUEL OIL a. Decane (C10H22) b. Dodecane (C12H26) c. Hexadecane (C16H34) d. Octadecane (C18H38) 2) Olefins - ends in "ylene" or "ene" Formula: CnH2n Structure: Chain (unsaturated) Example: a. Propene (C3H6) b. Butene (C4H8) c. Hexene ( C6H12) d. Octene ( C8H16) 3) DIOLEFIN - ends in "diene" Formula: CnH2n-2 Structure: Chain (unsaturated) Example: a. Butadiene (C4H6) b. Hexadiene (C6H10) 4) NAPHTHENE - named by adding the prefix "cyclo" Formula: CnH2n Structure: Ring (saturated) Example: a. Cyclopentane (C5H10) b. Cyclohexane (C6H12) 5) AROMATICS - this hydrocarbon includes the; A. Benzene Series (CnH2n-6) B. Naphthalene Series (CnH2n-12) Structure: Ring (unsaturated) Example: a. Benzene (C6H6) b. Toluene (C7H8) c. Xylene (C8H10) 6)ALCOHOLS - These are not true hydrocarbon, but sometimes used as fuel in an internal combustion engine. The characteristic feature is that one of the hydrogen atom is replaced by an OH radical. Example: a. Methanol (CH4O or CH3OH) b. Ethanol (C2H6O or C2H5OH) Covalent Bond: A molecular bond that involves the sharing of electron pairs between atoms. These electron pairs are known as shared pairs or bonding pairs, and the stable balance of ttractive and repulsive forces between atoms, when they share electrons, is known as covalent bonding. Ring Structure (Heterocyclic Compounds): It is a cyclic compounds that has atoms of at least two different elements as members of its ring(s). Heterocyclic chemistry is the branch of organic chemistry dealing with the synthesis, properties, and applications of these heterocycles. Chain Structure: A crystalline structure in which forces between atoms in one direction are greater than those in other directions, so that the atoms are concentrated in chains. Saturated Hydrocarbon – hydrocarbon that contain only single bonds between carbon atoms. They are the simplest class of hydrocarbons. They are called saturated because each carbon atom is bonded to as many hydrogen atoms as possible. All the carbon atoms are joined by a single bond. Unsaturated Hydrocarbon – are hydrocarbons that have double or triple covalent bonds between adjacent carbon atoms. Those with at least one carbon – to carbon double bond are called “alkenes” and those with at least one carbon – to – carbon triple bond are called “alkynes”.(it has two or more carbon atoms joined by a double or triple bond) Isomers – each of two or more compounds with the same formula but at different arrangement of atoms in the molecule and different properties.( two hydrocarbons with the same number of carbon and hydrogen atoms, but at different structure) STRUCTURE OF CnHm Complete Combustion: Occurs when all the combustible elements has been fully oxidized. C + O 2 → CO 2 Incomplete Combustion: Occurs when some of the combustible elements have not been fully oxidized and it may result from; a. Insufficient oxygen b. Poor mixing of fuel and oxygen c. the temperature is too low to support combustion. Result: Soot or black smoke that sometimes pours out from chimney or smokestack. C + 12 O 2 → CO 12 + 16 → 28 3+ 4 → 7 THE COMBUSTION CHEMISTRY A. Oxidation of Carbon C + O 2 → CO2 12 + 32 → 44 3 + 8 → 11 kgO 2 8 = kgC 3 B. Oxidation of Hydrogen H 2 + 12 O 2 → H 2O 2 + 16 → 18 1+ 8 → 9 kgO 2 8 = kgH 2 1 C. Oxidation of Sulfur S + O 2 → SO 2 32 + 32 → 64 1+1 → 2 kgO 2 1 = kgS 1 Composition of Air • • • • • • Oxygen. The most important gas in the composition is oxygen. ... Nitrogen. To balance out oxygen, there is Nitrogen. ... Argon. ... Carbon dioxide. ... Water vapor. ... Other Particles Gases Nitrogen Oxygen Argon Carbon Dioxide Water Vapor Other Particles % By Volume 78.09 20.95 0.93 0.04 1 (0.4% over the entire atmosphere) In theoretical Combustion, the composition of atmospheric air is considered as; a) Volumetric or Molal analysis O2 , = 21% N2 = 79% b) Gravimetric Analysis O2 = 23.3% N2 = 76.7% Moles of N 2 79 = = 3.76 Mole of O2 21 COMBUSTION WITH AIR and Theoretical air requirement Fuel + Air → Pr oducts A) Combustion of Carbon with air C + O 2 + 3.76 N 2 → CO2 + 3.76 N 2 12 + 32 + 3.76(28) → 44 + 3.76(28) kg of air = 11.44 kg of C B) Combustion of Hydrogen with Air H 2 + 12 O 2 + 12 (3.76) N 2 → H 2O + 12 (3.76) N 2 2 + 16 + 12 (3.76)(28) → 18 + 12 (3.76)(28) kg of air = 34.32 kg of H C) Combustion of Sulfur with air S + O 2 + (3.76) N 2 → SO2 + (3.76) N 2 32 + 32 + (3.76)(28) → 64 + (3.76)(28) kg of air = 4.29 kg of H THEORETICAL AIR The minimum amount of air that supplies sufficient oxygen for the complete combustion of all the carbon, hydrogen, and sulfur present in the fuel is called the theoretical amount of air kg of air A = F T heoretical Kg of Fuel EXCESS AIR It is an amount of air in excess of the theoretical air required to influence complete combustion. With excess air, O 2 is present in the products. Excess air is usually expressed as a percentage of the theoretical air. But in actual combustion, although there is an amount of excess air, the presence of CO and other emission gases in the products cannot be avoided. Example: 25% excess air is the same as 125% theoretical air. COMBUSTION OF HYDROCARBON FUEL(CnHm) A) Combustion of CnHm with 100% theoretical air C n H m + aO 2 + a (3.76) N 2 → bCO2 + cH 2O + a (3.76) N 2 By Carbon balance 1(n) = b b=n By Hydrogen balance 1(m) = 2c c = 0.5m By Oxygen balance 2a = 2b + c a = b + 0.5c a = n + 0.25m therefore for the combustion of one CnHm with 100% TA a = n + 0.25m b=n c = 0.5m 32a + a (3.28)28 137.28a A = = 12n + m 12n + m F T heoretical 137.28(n + 0.25m) A = 12n + m F T heoretical B) With excess air C n H m + (1 + e)aO 2 + (1 + e)a (3.76) N 2 → bCO2 + cH 2 O + dO 2 + (1 + e)a (3.76) N 2 By Oxygen balance 2(1 + e)a = 2b + c + 2d 2d = 2(1 + e)a - 2b - c d = (1 + e)a - b - 0.5c d = (1 + e)(n + 0.25m) − n − 0.25m d = n + 0.25m + en + e(0.25m) − n − 0.25m d = en + e(0.25m) d = e(n + 0.25m ) 137.28(1 + e)(n + 0.25m) kg of air A = → Actual A/F Ratio F 12n + m kg of C n H m Actual Note: The values of a,b,c, and d above in terms of n and m is applicable only for the combustion of one type of hydrocarbon. EQUIVALENCE RATIO ER = (F A) actual (F A)Stoichiometric Stoichiometric (or chemically correct) mixture of air and fuel, is one that contains just sufficient oxygen for complete combustion of the fuel A “Weak Mixture”, is one which has an excess of air A “Rich Mixture”, is one which has a deficiency of air Percentage Excess Air = (A F) ( F) − A (A F) Actual T heoretical T heoretical DEW POINT TEMPERATURE The Dew Point Temperature (tdp) is the saturation temperature corresponding the partial pressure of the water vapor in the mixture (products of combustion). ULTIMATE ANALYSIS Ultimate Analysis gives the amount of C, H2, O2, N2, S and moisture in percentages by mass, sometimes the percentage amount of Ash is given. O kg of air A = 11.44C + 34.32 H 2 − 2 + 4.29S 8 kg of fuel F t where: C, H, O and S are in decimals obtained from the Ultimate Analysis (on an ashless basis) PROXIMATE ANALYSIS Proximate Analysis gives the percentage amount of Fixed Carbon, Volatiles, Ash and Moisture. 100 % = %FC + %Volatiles + %Ash + %Moisture ORSAT ANALYSIS Orsat Analysis gives the volumetric or molal analysis of the products of combustion or exhaust gases on a Dry Basis. 100 % = %CO 2 + %O 2 + % N 2 + %CO + % NO x + %CH + ... MASS FLOW RATE OF FLUE GAS a) Without considering Ash loss: A mgas = mFuel + 1 F b) Considering Ash loss A mgas = mFuel + 1 − Ash Loss F where ash loss in decimal • Combustion equation with CO in the products due to incomplete combustion (100% theoretical air) CnHm + aO2 + a (3.76 ) N 2 → bCO 2 + cH 2O + dCO + a (3.76 ) N 2 • Combustion equation with CO in the products due to incomplete combustion (with excess air) CnHm + (1 + e)aO2 + (1 + e)a (3.76 ) N 2 → bCO 2 + cH 2O + dCO + fO 2 + (1 + e)a (3.76 ) N 2 • Typical Real-World Engine Combustion Process: Fuel (CnHm) + Air (O 2 and N 2 ) → CO2 + H 2O + O 2 + N 2 + CH(VOC's) + CO + NOx CH(VOC's) - Volatile Organic Compounds CO - Carbon Monoxide NOx - Nitrogen Oxides EMISSIONS Emissions are any kind of substance released into the air from natural or human sources — flows of gases, liquid droplets or solid particles. Not all emissions become air pollutants, but many do, causing significant health and environmental problems. The amount of air pollutants in an area depends on the number and size of emission sources, along with the weather and lay of the land. The main sources of emissions are: ❖ Point Sources Point sources are stationary industrial facilities such as pulp and paper mills and factories that burn fossil fuels. They operate under ministry authorization (a regulation, permit, approval, or code of conduct), or under an air-discharge permit issued by Philippine Govt. ❖ Area Sources Area sources are stationary sources that are not normally required to obtain a discharge permit from the ministry. They include prescribed burning, residential wood use, light industry, and other residential, commercial and institutional sources. Emissions from most of these area sources individually are small compared to point sources, but can be significant when considered collectively. ❖ Mobile Sources Mobile sources include motor vehicles mainly involved in the transportation of people and goods (e.g., passenger cars, trucks and motorcycles), aircraft, marine vessels, trains, off-road vehicles, and small off-road engines (e.g., agricultural, lawn/garden, construction and recreational equipment). ❖ Natural Sources Natural sources of emissions occur in nature without the influence of human beings, such as wildfires, plants, wildlife and marine aerosol. Pollutants: Air pollutants are any gas, liquid or solid substance that have been emitted into the atmosphere and are in high enough concentrations to be considered harmful to the environment, or human, animal and plant health. Pollutants emitted directly into the air are called "primary pollutants." "Secondary" pollutants" are formed in the air, when they react with other pollutants. Ground-level ozone is an example of a secondary pollutant that forms when nitrogen oxides (NOx) and volatile organic compounds (VOCs) react in the presence of sunlight. We come in contact with many kinds of air pollutants every day. Depending on the type and amount emitted, these pollutants may affect air quality at the local, regional, and/or global scale. For example, smoke from woodstoves or backyard burning, and motor vehicle exhaust are pollutant mixtures that affect air quality in our neighborhoods and communities, and inside our homes. Smoke from forest fires or ground-level ozone can cover an entire region. Long-lasting pollutants can contribute to serious global problems, such as ozone depletion and climate change. An air pollutant can become dangerous to our health when we are exposed to it for a long time, and also when we breathe in a large amount of it. Health effects can last for a short while (e.g., coughing) or become a long-term problem (e.g., lung and heart disease, cancer). Pollution can also cause death. The young, the elderly and those with pre-existing heart or lung disease are the most sensitive to the effects of air pollution. Common Pollutants Air pollutants can be visible (e.g., the brownish-yellow colour of smog) or invisible. Besides affecting human health and the environment, air pollutants can also hamper our ability to see very far (visibility). Air pollution can have local and regional impacts — such as ground-level ozone and wood smoke. It can also have widereaching, global effects — such as climate change and depletion of the ozone layer. Health effects from local air pollution can last for a short while (e.g., coughing) or become a long-term problem (e.g., lung and heart disease, cancer). Pollution can also cause death. An air pollutant can become dangerous to our health when we are exposed to it for a long time, as well as when we breathe in a large amount of it. The Most Significant Air Pollutants The air pollutants that pose the most serious local threat to our health are particulate matter and ground-level ozone — the key ingredients of smog. They mainly affect the lowest part of the atmosphere, which holds the air we breathe. Particulate matter is a significant problem in rural areas, as well, due to wood burning. Particulate Matter (PM) Particulate matter refers to tiny solid or liquid particles that float in the air. Some particles are large or dark enough to be seen as smoke, soot or dust. Others are so small that they can only be detected with a powerful, electron microscope. PM occurs in two forms: primary and secondary. • Primary PM is emitted directly into the atmosphere by wood burning (e.g., in wood stoves, open burning, wood stoves) and fossil fuel burning (e.g., in motor vehicles, oil/gas furnaces and industry). Primary PM also includes pollen, spores and road dust. • Secondary PM is formed in the atmosphere through chemical reactions involving nitrogen dioxide, sulphur dioxide, volatile organic compounds and ammonia. We measure particulate matter in microns (micrometres). One micron is a millionth of a metre. Particulate matter between 10 and 2.5 microns in diameter or less is called PM10. That’s about seven times smaller than the width of a human hair. It is invisible to the naked eye and small enough to inhaled into our nose and throat. Particulate matter that’s 2.5 microns and less is called PM2.5. This is the particulate matter of greatest concern because it can travel deep into the lungs and become lodged there, causing heart and lung disease, and premature death. Fine particles that comprise PM2.5 are also efficient at scattering light, resulting in a degradation in visibility. Ground-Level Ozone (O3) Ground-level ozone is formed by the reaction of two types of chemicals — volatile organic compounds and nitrogen oxide — in the presence of sunshine and warm temperatures. When the air is still (stagnant), the ozone will build up. Ground-level ozone usually occurs in the warmer months of the year. Ground-level ozone collects over urban areas that produce large amounts of VOCs and NOx. Rural areas can be affected, too, though. That’s because the ozone can travel up to several hundred kilometres away, carried by the wind. Low concentrations of ground-level ozone can irritate the eyes, nose and throat. Ozone can also irritate the lung airways, and make them red and swollen (inflammation). People with lung problems are most at risk, but even healthy people who are active outdoors can be affected when ozone levels are high. EXHAUST POLLUTANTS HYDROCARBONS (HC): Hydrocarbon emissions result when fuel molecules in the engine do not burn or burn only partially. Hydrocarbons react in the presence of nitrogen oxides and sunlight to form ground-level ozone, a major component of smog. Ozone can irritate the eyes, damage lungs, and aggravate respiratory problems. It is our most widespread urban air pollution problem. Some kinds of exhaust hydrocarbons are also toxic, with the potential to cause cancer. NITROGEN OXIDES (NOx): Under the high pressure and high temperature conditions in an engine, nitrogen and oxygen atoms in the air we breathe react to form various nitrogen oxides, collectively known as NOx. Nitrogen oxides, like hydrocarbons, are precursors to the formation of ozone. They also contribute to the formation of acid rain. CARBON MONOXIDE (CO): Carbon monoxide is a product of incomplete combustion and occurs when carbon in the fuel is partially oxidized rather than fully oxidized to carbon dioxide. Carbon monoxide reduces the flow of oxygen in the bloodstream and is particularly dangerous to persons with heart disease. CARBON DIOXIDE (CO2): Carbon dioxide does not directly impair human health, but it is considered a “greenhouse gas”. In other words, as it accumulates in the atmosphere, it is believed to trap the earth’s heat and contribute to the potential for climate change. Evaporative Emissions HYDROCARBONS: Hydrocarbons also escape into the air through fuel evaporation. With today’s efficient exhaust emission controls and today’s clean burning gasoline formulations, evaporative losses can account for a majority of the total hydrocarbon pollution from current model cars on hot days when ozone levels are highest. Evaporative emissions occur from fuel. OTHER KINDS OF AIR POLLUTANTS There are many more air pollutants than particulate matter and ground-level ozone. They are usually grouped into four categories, as shown in the table below. Pollutant Category Types of Pollutants Common Air Contaminants(CACs) (also known as "criteria air contaminants") particulate matter (PM), sulphur oxides (SOx), nitrogen oxides (NOx), volatile organic compounds (VOCs), carbon monoxide (CO) and ammonia (NH3). Ground-level ozone (O3) is often included with CACs because it is a byproduct of CAC interactions. Persistent Organic Pollutants(POPs) e.g., dioxins and furans Heavy Metals e.g., mercury Air Toxics e.g., benzene, polycyclic aromatic hydrocarbons(PAHs) Table of Common Pollutants Not included here are the pollutants that influence the larger atmosphere, causing global environmental problems: stratospheric ozone depletion and global climate change. MAIN (COMMON) POLLUTANTS Pollutant Description and Sources Health Impact Environment Particulate Matter (PM) Dust, soot, and tiny bits of solid material. PM10 — Particles smaller than 10µm (microns) in diameter. Far too small to see — 1/8th the width of a human hair. • Road dust; road construction • Mixing and applying fertilizers/ pesticides • Forest fires • Coarse particles irritate the nose and throat, but do not normally penetrate deep into the lungs. haze that reduces visibility. • PM is the main source of • It takes hours to days for PM10 to settle out of the air. • Because they are so small, PM2.5 stays in the air much longer than PM10, taking days to weeks to be removed. • PM can make lakes and other sensitive areas more acidic, causing changes to the nutrient balance and harming aquatic life. PM2.5–Particles smaller than 2.5µm in diameter fireplaces) • Combustion of fossil fuels and wood (motor vehicles, woodstoves and • Industrial activity • Garbage incineration • Agricultural burning • Fine particles are small enough to make their way deep into the lungs. They are associated with all sorts of health problems — from a runny nose and coughing, to bronchitis, asthma, emphysema, pneumonia, heart disease, and even premature death. • PM2.5 is the worst public health problem from air pollution in the province. (Research indicates the number of hospital visits increases on days with increased PM levels). Ground level Ozone (O3) Bluish gas with a pungent odour • At ground level, ozone is formed by chemical reactions between volatile organic compounds (VOCs) and nitrogen dioxide (NO2) in the presence of sunlight. • VOCs and NO2 are released by burning coal, gasoline, and other fuels; and naturally by plants and trees. • Exposure for 6-7 hours, even at low concentrations, significantly reduces lung function and causes respiratory inflammation in healthy people during periods of moderate exercise. Can be accompanied by symptoms such as chest pain, coughing, nausea, and pulmonary congestion. Impacts on individuals with pre-existing heart or respiratory conditions can be very serious. • Ozone exposure can contribute to asthma, and reduced resistance to colds and other infections. plants and trees, leading to reduced yields. • Ozone can damage • Leads to lung and respiratory damage in animals. • Ozone can also be good: the ozone layer above the earth (the stratosphere) protects us from harmful ultraviolet rays. Other Pollutants • sulphur dioxide (SO2) • carbon monoxide (CO) • nitrogen dioxide (NO2) • total reduced sulphur (TRS) • volatile organic compounds (VOCs) • persistent organic pollutants (POPs) • lead (Pb) • polycyclic aromatic hydrocarbons (PAHs) • dioxins and furans Most of these pollutants come from combustion and industrial processes or the evaporation of paints and common chemical products. • The health impacts of these pollutants are varied. • Sulphur dioxide (SO2), for example, can transform in the atmosphere to sulphuric acid, a major component of acid rain. • Carbon monoxide is fatal at high concentrations, and causes illness at lower concentrations. • Dioxins and furans are among the most toxic chemicals in the world. • While some of these pollutants have local impact on the environment (e.g., lead) or are relatively short lived (NO2) some are long lived (POPs) and can travel the world on wind currents in the upper atmosphere. Combustion of Hydrocarbon Fuel a) With 100% theoretical air C n H m + aO2 + a (3.76) N 2 → bCO2 + cH 2O + a (3.76) N 2 where a = n + 0.25m b=n c = 0.5m b) With excess air e C n H m + (1 + e)aO2 + (1 + e)a (3.76) N 2 → bCO2 + cH 2O + dO2 + (1 + e)a (3.76) N 2 where d = e(n + 0.25m) c) With exhaust pollutants (emission gases) CnHm + aO 2 + a(3.76)N2 ) → bCO2 + cH 2 O + dO 2 + fN 2 + gCH + hCO + iNOx CH(VOC's) - Volatile Organic Compounds CO - Carbon Monoxide NOx - Nitrogen Oxides Note : The above values of a, b, c and d in terms of n and m may not apply to actual combustion process Combustion of Solid Fuels a) Combustion with 100% theoretical air aC + bH 2 + cO2 + dN 2 + fS + gH 2O + xO 2 + x (3.76 ) N 2 → hCO 2 + iH 2O + jSO 2 + kN 2 b) Combustion with Excess air e aC + bH 2 + cO 2 + dN 2 + fS + gH 2 O + (1 + e) xO 2 + (1 + e) x (3.76) N 2 → hCO 2 + iH 2 O + jSO 2 + LO 2 + mN 2 c) Combustion with exhaust pollutants (emission gases) aC + bH 2 + cO2 + dN 2 + fS + gH 2O + (1 + e)xO 2 + (1 + e)x(3.76) N 2 → hCO 2 + iH 2O + jSO 2 + LO 2 + mN 2 + nCO + oCH + pNOx Note: In balancing combustion equation for Solid fuels, convert the Ultimate Analysis of Coal to Molal or volumetric analysis, then reduced to and Ashless basis Example: Reduction of Ultimate coal analysis to Molal ashless analysis Kg of CO2 per kg of C formed C + O 2 → CO 2 12 + 32 → 44 3 + 8 → 11 kg of CO 2 11 = kg of C 3 Kg of H2O per kg of H formed H2 + 1 2 O2 → H 2O 2 + 16 → 18 1+ 8 → 9 kg of H 2 O 9 = kg of H 1 Kg of SO2 per kg of S formed S + O 2 → SO 2 32 + 32 → 64 1+1 → 2 kg of SO 2 2 = kg of S 1 Total Mass of Products m Pr oducts = ΣniMi m Pr oducts = n CO 2 M CO 2 + n H 2O M H 2O + n O 2 M O 2 + n SO 2 M SO 2 + n N 2 M N 2 + n CO M CO + n CH M CH + n NOx M NOx Total Moles of Products n Pr oducts = Σni n Pr oducts = n CO 2 + n H 2O + n O2 + nSO 2 + n N 2 + n CO + n CH + n NOx Dew Point Temperature t dp = ( tsat ) Saturation temperatu re corresponding the partial pressure of H 2 O (PH 2O ) PH 2O = (P) n H 2O n Products P = total pressure of product Moles of Dry Flue Gas (The H2O is not included in the analysis) n Dry Flue Gas = nCO2 + nO2 + nSO 2 + n N2 + nCO + nCH + n NOx % of CO2 in the dry flue gas n CO 2 n CO 2 x 100% = x 100% n Dry Flue Gas n CO 2 + n O2 + nSO 2 + n N 2 + n CO + n CH + n NOx Total Mass of Fuel a. For Hydrocarbon of Hydrocarbon Mixture m Fuel = Σn F M F b. For Solid Fuels mFuel = ΣniMi mFuel = n CMC + n H 2MH 2 + n O2MO2 + n N 2M N 2 + nSMS + n H 2OMH 2O Mass Flow Rate of Products (Known Fuel flow rate) kg m kg of Products = Products x Fuel Flow Rate hr mFuel hr Volume of Products at the product Pressure and Temperature (m 3) VPr oducts = n Pr oducts (R )T 3 m P Volume flow rate of Products at the product Pressure and Temperature (m 3/hr) m3 V m3 of Products = Products x Fuel Flow Rate hr mFuel hr Molecular Weight of Products M= n CO 2 M CO 2 + n H 2O M H 2O + n O 2 M O 2 + n SO 2 MSO 2 + n CO M CO + n CH M CH + n NOx M NOx + n N 2 M N 2 + ...n i M n Pr oducts Gas Constant of Products 8.3143 KJ M kg - K Σ(niMi )Ri R = ΣxiRi = Σ(niMi ) R= Specific Heat of Products Cp = Σx iCpi Cv = Σx iC vi R = Cp − C v k= Cp Cv Rk KJ k − 1 kg - K R KJ Cv = k − 1 kg - K Cp = Example No. 1: In the figure below, Determine a. Percent excess air b. Volumetric Analysis of Products c. Orsat Analysis mp = ma + mF m p = 4000 + 200 = 4,200 kg hr 4000 A = = 20 F Actual 200 A A = (1 + e ) F Actual F T heoretical A F Actual − 1 e= A F T heoretical CH 4 + aO 2 + a (3.76) N 2 → bCO2 + cH 2 O + a (3.76) N 2 ( ) ( ) 137.27(n + 0.25m) A = = 17.16 12n + m F T heoretical e = 0.17 = 17% Combustion with EA; e = 0.17 CH 4 + (1.17)aO 2 + (1.17)a (3.76) N 2 → bCO2 + cH 2 O + dO 2 + (1.17)a (3.76) N 2 a = n + 0.25m = 2.34 b = n =1 c = 0.5m = 2 d = e(n + 0.25m) = 0.34 CH 4 + 2.34O 2 + 8.8N 2 → 1CO2 + 2H 2 O + 0.34O 2 + 8.8N 2 n Pr oducts = 1 + +2 + 0.34 + 8.8 = 12.14 Pr oduct Analysis y CO 2 = 8.24%; y H 2 O = 16.48%; y O 2 = 2.8%; y N 2 = 72.48% n Dry Pr oducts = 1 + 0.34 + 8.8 = 10.14 Orsat Analysis y CO 2 = 9.86% y O 2 = 3.35% y N 2 = 86.78% Example No. 2 (Combustion of Gasoline) Typical gasoline C8H18 is burned with 20% excess air by weight. Find a. the air-fuel ratio b. the percentage CO2 by volume in the dry exhaust gases c. kg of water vapor formed per kg of fuel d. volume of dry exhaust gas per kg of fuel if T = 290 K and P = 101.33 KPa e. the partial pressure of the water vapor in the exhaust f. the dew point temperature of the products Fuel: C8H18 Excess air: e = 20% Product Temperature = 290 K Product Pressure = 101.33 KPa Combustion with 100% theoretical air C8H18 + aO2 + a (3.76) N2 → bCO2 + cH2O + a (3.76) N2 C8H18 + 12.5O2 + 47N2 → 8CO2 + 9H2O + 47N2 Combustion with e = 20% C8H18 + (1.20)12.5O2 + (1.20)47N2 → 8CO2 + 9H2O + dO2 + (1.20)47N2 C8H18 + 15O2 + 56.4N2 → 8CO2 + 9H2O + 2.5O2 + 56.4N2 → Actual Combustion eq. a. Actual Air – Fuel Ratio 15(32) + (56.4)(28) A = = 18.06 F 12(8) + 1(18) ACT UAL b. the percentage CO2 by volume in the dry exhaust gases n d − moles of dry exhaust gas n d = 8 + 2.5 + 56.4 = 66.9 8 x100% = 11.95% 66.9 c. kg of water vapor formed per kg of fuel y CO 2 = n − moles of exhaust gas n d = 8 + 9 + 2.5 + 56.4 = 75.9 kg H 2O = 9(18) = 162 kg kg H 2O 162 162 kg = = = 1.42 kg C8H18 12(8) + 1(18) 114 kg d. volume of dry exhaust gas per kg of fuel if T = 290 K and P = 101.33 KPa n d − moles of dry exhaust gas n d = 8 + 2.5 + 56.4 = 66.9 PV = n RT 66.9(8.3143)(290) 3 Vd = m 101.33 Vd = 1,591.9 m3 1,591.9 m3 = 14 kgC8H18 114 kgC8H18 e. the partial pressure of the water vapor in the exhaust n − moles of exhaust gas Vd = n = 8 + 9 + 2.5 + 56.4 = 75.9 9 y H 2O = x100% = 11.86% 75.9 P y H 2O = H 2O P PH 2O = 0.1186(101.33) = 12.015 KPa f. the dew point temperature of the products DPT = saturation temperatu re corresponding PH 2O PH 2O = 12.015 KPa From Steam Table DPT = 46.467C if the mixture is cooled below DPT, condensati on of H 2O in the mixture will occur Example No. 3 (Known Orsat analysis and Fuel) A fuel oil C12H26 is used in an internal combustion engine and the Orsat analysis are as follows: CO 2 = 12.8% ; O2 = 3.5%; CO = 0.2% and N2 = 83.5%. Determine the actual air-fuel ratio and the percent excess air. Solution: (Basis 100 moles of dry flue gas and a moles of fuel) aC12H26 + bO2 + b(3.76)N2 → 12.8CO2 + cH2O + 0.2CO + 3.5O2 + 83.5N2 By C balance 12a = 12.8 + 0.2 a = 1.0833 By N2 Balance b(3.76) = 83.5 b = 22.207 By H balance 26a = 2c c = 26(1.0833)/2 c = 14.083 aC12H 26 + bO 2 + b(3.76)N2 → 12.8CO2 + cH 2O + 0.2CO + 3.5O2 + 83.5N2 dividing the equation by a C12H 26 + 20.5O2 + 77.08N2 → 11.816CO2 + 13H 2 O + 0.185CO + 3.23O2 + 77.08N2 20.5(32) + (77.08)(28) A = = 16.56 12(12) + 1(26) F Actual Theoretica l Air - Fuel Ratio 137.28(n + 0.25m) A = = 14.94 F 12n + m T heroretical A F Actual − 1 = 0.108 = 10.8% e= A F T heoreical ( ) ( ) Example No. 4 (Gasoline with Orsat analysis) The following is the ultimate analysis of a sample of petrol by weight : C = 84.2 % ; H = 15.8 %. Calculate the ratio of air to petrol consumption by weight if the volumetric analysis of the dry exhaust gas is :CO 2 = 11.07 % ; CO = 1.23 % ; O2 = 3.72 % ; N2 = 83.97 %. Also find percentage excess air. 12n %C = 12n + m 12n 0.842 = 12n + m 12 12n + m = n = 14.25n → eq.1 0.842 m %H = 12n + m m 0.158 = 12n + m 1 12n + m = m = 6.33m → eq.2 0.158 14.25n = 6.33m m = 2.25n → eq.3 For petrol Fuel the formula is C n H 2n + 2 m = 2n + 2 2.25n = 2n + 2 n =8 m = 18 137.28(n + 0.25m) A = = 14.57 12n + m F T heoretical Combustion Equation (Basis 100 moles of dry flue gas) C8 H18 + aO 2 + bN 2 → 11.07CO2 + cH 2 O + 1.23CO + 3.72O 2 + 83.97 N 2 b = 83.97 a (3.76) = b a = 22.33 c = 13.84 32a + 28b A = = 17.49 F Actual 12n + m 17.49 e= − 1 = 0.162 = 16.2% 14.57 Example No. 5 (Coal Fuel) The following data were obtained from a boiler test: Ultimate analysis of coal as fired is; C = 62%, H2 = 4%, O2 = 8%, N2 = 1 %, S = 2%, H2O = 8% and Ash = 15%. Excess air is 25% for complete combustion. Fuel and air temperature and pressure are, 25C and 101 KPa, respectively. Flue gas temperature is 300C and P = 101 KPa. Determine a. Ultimate analysis on an ashless basis b. Molal analysis of fuel on an ashless basis c. Combustion equation d. Actual air – fuel ratio in kg/kg e. Volumetric Analysis of Products f. Molecular Weight and Gas Constant of Products g. Cubic meter of CO2 per kg of fuel burnt h. Cubic meter of SO2 per kg of fuel burnt Ashless U.A. C =72.9% ; H2 = 4.7% ; O2 = 9.4% ; N2 = 1.2% ; S = 2.4% ; M = 9.4% Molal analysis on an ashless basis C =64.91% ; H2 = 25.13% ; O2 = 3.14% ; N2 = 0.45% ; S = 0.79% ; H2O = 5.58% Combustion equation w ith 100 TA 64.91C + 25.13H2 + 3.14O2 + 0.45N2 + 0.79S + 5.58H2O → Fuel aO 2 + a(3.76)N2 → Air bCO2 + cH 2O + dSO2 + eN 2 → Products 64.91C + 25.13H2 + 3.14O2 + 0.45N2 + 0.79S + 5.58H2O → Fuel 75.12O2 + 282.46 N 2 → Air 64.91CO2 + 30.71H 2O + 0.79SO 2 + 282.91N 2 → Products Combustion equation w ith 25% E.A. 64.91C + 25.13H2 + 3.14O2 + 0.45N2 + 0.79S + 5.58H2O → Fuel (1.25)75.12O 2 + (1.25)282.46 N 2 → Air 64.91CO2 + 30.71H 2O + 0.79SO 2 + fO 2 + gN 2 → Products 2(3.14) + (5.58) + (1.25)75.12(2) = 2(64.91) + 30.71 + 2(0.79) + 2f f = 18.78 2(0.45) + 2(1.25)282.46 = 2g g = 353.52 64.91C + 25.13H2 + 3.14O2 + 0.45N2 + 0.79S + 5.58H2O → Fuel 93.9O2 + 353.07 N 2 → Air 64.91CO2 + 30.71H 2O + 0.79SO 2 + 18.78O 2 + 353.52 N 2 → Products 32(93.9) + 28(353.07) A = = 12.07 F Actual 12(64.91) + 2(25.13) + 32(3.14) + 28(0.45) + 32(0.79) + 18(5.58) yi = ni n n Pr oducts = 64.91 + 30.71 + 0.79 + 18.78 + 353.52 = 468.71 64.91 x100% = 13.85% 468.71 30.71 y H 2O = x100% = 6.55% 468.71 0.79 ySO 2 = x100% = 0.17% 468.71 18.78 yO2 = x100% = 4.01% 468.71 353.52 y N2 = x100% = 75.42% 468.71 y CO 2 = M = ΣyiMi 64.91(44) + 30.71(18) + 0.79(64) + 18.78(32) + 353.52(28) kg M= = 29.78 468.71 kgm 8.3143 KJ R= = 0.279 M kg - K PV = n RT n RT P (64.91)(8.3143)(300 + 273) VCO 2 = = 3061.91 m3 101 VCO 2 3061.91 m3 = = 2.87 kg of Fuel 12(64.91) + 2(25.13) + 32(3.14) + 28(0.45) + 32(0.79) + 18(5.58) kg of Fuel (0.79)(8.3143)(300 + 273) VSO 2 = = 37.04 m 3 101 VSO 2 37.04 m3 = = 0.03 kg of Fuel 12(64.91) + 2(25.13) + 32(3.14) + 28(0.45) + 32(0.79) + 18(5.58) kg of Fuel V= Example No. 6 (Alcohol) Calculate the theoretical Oxygen/fuel ratio and Air/fuel ratio on a mass basis for the combustion of ethanol, C2H5OH. C 2 H 5OH + aO2 + a (3.76) N 2 → bCO2 + cH 2O + a (3.76) N 2 2=b 6 = 2c c=3 1 + 2a = 2b + c a =3 Combustion Equation C 2 H 5OH + 3O 2 + 11.28N 2 → 2CO2 + 3H 2O + 11.28N 2 A 3(32) + 11.28(28) = = 8.95 F 46 O2 32(3) kg = = 2.09 Fuel 46 kg Example No. 7 (Gaseous Fuel Mixture) A gaseous fuel mixture has the following volumetric analysis, CH4 = 60% ; CO = 30% and O2 = 10% If this fuel is burned with 30% excess air by volume, determine a. The combustion equation b. The actual fuel ratio c. The Orsat analysis d. The dew point temperature (assume P = 101.325 KPa) Combustion Equation Combustion with 100% TA 60CH 4 + 30CO + 10O 2 + aO 2 + a (3.76) N 2 → bCO2 + cH 2 O + O 2 + a (3.76) N 2 a = 125 b = 90 c = 120 Combustion with 305 EA 60CH 4 + 30CO + 10O 2 + (1.30)aO 2 + (1.30)a (3.76) N 2 → 90CO2 + 120H 2 O + dO 2 + (1.30)a (3.76) N 2 d = 37.5 60CH 4 + 30CO + 10O 2 + 162.5O 2 + 611N 2 → 90CO2 + 120H 2 O + 37.5O 2 + 611N 2 A 162.5(32) + 611(28) = = 11.52 F 60(16) + 30(28) + 10(32) n Products = 90 + 120 + 37.5 + 611 = 858.5 ni x100% n Volumetric Analysis of Products y CO2 = 10.48% yi = y H 2O = 13.98% y O2 = 4.37% y N2 = 71.17% Pi P PH20 = 0.1398(101.325) = 14.16 KPa DPT = 52.8C ORSAT ANALYSIS n Dry Gas = 858.5 − 120 = 738.5 yi = y CO2 = 12.2% y O2 = 5.1% y N2 = 82.7% Example No. 8 (Producer’s Gas) Producer gas from bituminous coal contains following molar analysis. CH4 = 3 % , H2 = 14.0%, N2 = 50.9%, O2 = 0.6%, CO = 27.0% and CO2 = 4.5%. This is burned with 25% excess air, Calculate the air/fuel ratio on a volumetric basis and on a mass basis. 3CH4 + 14H 2 + 50.9 N 2 + 0.6O2 + 27CO + 4.5CO2 + 32.38O2 + 121.73N 2 → 34.5CO2 + 20H 2O + 6.48O2 + 172.63N 2 A kg = 1.8 F kg A mol = 1.54 F mol Example No. 9 (Combustion with emission gas) An combustor of a small scale industrial plant burns liquid Octane (C3 H8 ) at the rate of 0.005 kg/sec, and uses 20% excess air. The air and fuel enters the engine at 25C and the combustion products leaves the engine at 900 K. It may be assumed that 90% of the carbon in the fuel burns to form CO 2 and the remaining 1.5% burns to form CO.(P = 101 KPa) Determine a. The actual air – fuel ratio b. The kg/s of actual air per hour c. The M and R of the products d. The m3/sec of products at the product temperature and pressure e. The cubic meter of CO emission for 24 hrs operation Combustion with 100% theoretical air Combustion with 100% TA and CO emission C3H 8 + aO 2 + a(3.76)N2 → bCO2 + cH 2 O + dCO + a(3.76)N2 d = 0.015(3) = 0.045 b = 3 − 0.045 = 2.955 1(8) = 2c c=4 2a = 2b + c + d a = 4.978 C3H 8 + 4.978O 2 + 18.715N 2 → 2.955CO2 + 4H 2 O + dCO + 18.715N 2 Combustion with 20% EA C3H 8 + (1.20)4.978O 2 + (1.20)18.715N 2 → 2.955CO2 + 4H 2 O + 0.045CO + fO 2 + (1.20)18.715N 2 By oxygen balance f = 0.996 COMBUSTION EQUATION C3H 8 + 5.973O 2 + 22.458N 2 → 2.955CO2 + 4H 2 O + 0.045CO + 0.996O 2 + 22.458N 2 Actual Air - Fuel Ratio 5.973(32) + (22.458)( 28) A = = 18.64 F 12(3) + 1(8) Actual kg Mass of air = 18.64(0.005)(3600) = 335.444 hr Moles of Products = 2.955 + 4 + 0.045 + 0.996 + 22.458 = 30.45 moles M = ΣyiMi ni yi = n 2.955(44) + 4(18) + 0.045(28) + 0.996(32) + 22.458(28) M = ΣyiMi = 30.45 kg M = 28.37 kgm 8.3143 KJ R= = 0.293 28.37 kg - K PV = n RT m3 n RT m Fuel 30.45(8.3143)(900)(0.005) m3 = of Products = = 0.26 sec P 12(3) + 1(8) 101(44) sec m3 n RT m Fuel 0.045(8.3143)(900)(0.005)(3600) m3 = of CO = = 1.4 hr P 12(3) + 1(8) 101(44) sec Example No. 10 (Hydrocarbon Fuel) A hydrocarbon fuel represented by C12H26 is used as fuel in an IC engine and requires 25 % excess air for complete combustion. Determine a. The combustion equation b. The theoretical air – fuel ratio c. The actual air – fuel ratio d. The volumetric and gravimetric analysis of the products e. The molecular weight M and gas constant R of the products f. The kg of CO2 formed per kg of fuel g. % C and %H in the fuel Solution Fuel: C12H26 Combustion with 100% theoretical air With 100% TA C12H 26 + aO 2 + a (3.76) N 2 → bCO2 + cH 2 O + a(3.76)N 2 Carbon balance b=n Hydrogen balance m = 0.5m Oxygen balance a = n + 0.25m With 25% EA C12H 26 + (1 + e)aO 2 + (1 + e)a (3.76) N 2 → bCO2 + cH 2 O + dO 2 + (1 + e)a(3.76)N 2 d = e(n + 0.25m) COMBUSTION EQUATION C12H 26 + 23.125O 2 + 86.950N 2 → 12CO2 + 13H 2 O + 4.625O 2 + 86.950N 2 Products Gases Mi ni yi mi xi yiMi yi(%) xi(%) CO2 44 12 0.103 528 0.158 4.529 10.3 15.8 H2O 18 13 0.112 234 0.070 2.007 11.2 7.0 O2 32 4.625 0.040 148 0.044 1.270 4.0 4.4 N2 total 28 86.95 0.746 2434.6 0.728 20.884 74.6 72.8 116.575 1.00 3344.6 1.00 28.691 100.0 100.0 The combustion equation C12H 26 + 23 .125 O 2 + 86 .95 N 2 → 12CO 2 + 13H 2 O + 4.625O 2 + 86 .95 N 2 The theoretical A/F ratio 137.28(n + 0.25m) kg of air A = = 14.94 12n + m kg of C12H 26 F T heoretical The actual A/F ratio kg of air A A = (1 + e) = 18.674 F F kg of C12H 26 Actual t The Volumetric and gravimetric Analysis Gases yi(%) xi(%) CO2 10.3 15.8 H2O 11.2 7.0 O2 4.0 4.4 N2 total 74.6 72.8 100.0 100.0 Molecular weight and Gas constant kg M = ΣyiMi = 28.691 kg m R = ΣxiRi M 8.3143 KJ R= = 0.2898 28.691 kg - K R= Kg of CO2 per kg of fuel kg of CO2 528 = = 3.106 kg of C12H 26 12(12) + 26 % C and % H in the fuel 12n x 100% 12n + m 12(12) %C = x 100 = 84.7% 12(12) + 26 m %H = x 100% 12n + m 26 %H = x 100 = 15.3% 12(12) + 26 %C = COMBUSTION ENGINERING SAMPLE EXERCISES Example No. 1 (Coal Fuel) In a furnace. 500 kg of coal with an Ultimate analysis of C = 78 %, H2 =5 %, O2 = 8 %, S = 1%, M = 2% and an A = 6 % is fully consumed hourly with 30% excess air. How much air must be fed into the furnace, and how much flue gas is produced in kg/hr. Converting the UA on an ashless basis, then to molal ashless analysis Fuel U.A.% C H2 O2 N2 S H2O Ash 78 5 8 0 1 2 6 100 94% Ashless U.A. Ashless 83.0 5.3 8.5 0.0 1.1 2.1 100 Mi xi/Mi 12 2 32 28 32 18 - 0.069 0.027 0.003 0.0003 0.0012 0.0999 Molal Analysis 69.21 26.62 2.66 0.33 1.18 100 Combustion with 100% TA Basis 100 moles of fuel 69.21C + 26.62H 2 + 2.66O 2 + 0.33S + 1.18H 2 O + xO 2 + x (3.76) N 2 → Air + Fuel aCO2 + bH2O + cSO2 + dN2 → Pr oducts Carbon Balance 69.21 = a a = 69.21 Hydrogen Balance 26.62(2) + 1.18(2) = 2b b = 27.8 Sulfur Balance 0.33 = c Oxygen Balance 2.66(2) + 1.18(2) + 2x = 2a + b + 2c x = 104.24 Nitrogen Balance d = 301.50 Combustion with EA(0.30) 69.21C + 26.62H 2 + 2.66O 2 + 0.33S + 1.18H 2 O + (1.30) xO 2 + (1.30) x (3.76) N 2 → Air + Fuel aCO2 + bH 2 O + cSO2 + eO 2 + fN 2 → Pr oducts By oxygen blance e = 24.06 Nitrogen balance f = 391.94 104.24(32) + 391.94(28) A = = 14.30 F Actual 69.21(12) + 26.62(2) + 2.66(32) + 0.33(32) + 1.18(18) kg m air = 14.30(500) = 7,149.24 hr kg Flue Gas 69.21(44) + 27.8(18) + 0.33(64) + 24.06(32) + 391.94(28) = = 15.3 69.21(12) + 26.62(2) + 2.66(32) + 0.33(32) + 1.18(18) kg Fuel m Pr oducts = 15.3(500) = 7,649.24 kg hr Example No. 2(Hydrocarbon mixture with emission) A fuel mixture with a molal analysis of 50% C7H16 and 50% C8 H18 is oxidized with 30% excess air. If 15 moles of the carbon atoms oxidizes to CO and 10 of Nitrogen atoms goes to NO, Determine a. the combustion equation b. the actual air fuel ratio c. the cubic meter of exhaust pollutants formed per kg of fuel at P = 101 KPa and t = 900C d. the Orsat analysis of the products Combustion with 100% TA Basis :100 moles of fuel 50C7 H16 + 50C8 H18 + aO 2 + a(3.76)N 2 → bCO2 + cH 2 O + 15CO + 10NO + fN 2 Carbon Balance 50(7) + 50(8) = b + 15 b = 735 Hydrogen Balance 50(16) + 50(18) = 2c c = 850 Oxygen Balance 2a = 2(735) + 850 + 15 + 10 a = 1172.50 Combustion with excess air (30%) 50C7 H16 + 50C8 H18 + (1.30)aO 2 + (1.30)a(3.76)N 2 → bCO2 + cH 2 O + 15CO + 10NO + gO 2 + hN 2 By oxygen balance g = 351.75 by Nitrogen balance h = 5726.18 Combustion Equation 50C7 H16 + 50C8 H18 + 1524.25O 2 + 5731.18N 2 → 735CO2 + 850H 2 O + 15CO + 10NO + 351.75O 2 + 5726.18N 2 1524.25(32) + 5731.18(28) A = 19.56 Actual = F 50(100) + 50(114) nPollu tan t = 735 + 15 + 10 = 760 moles n RT 760(8.3143)(900 + 273) = = 73,386.46 m 3 of exhaust pollutant P 101 m 3 of exhaust pollutant 73,386.46 = = 6.86 kg of Fuel 50(100) + 50(114) n Dry Flue Gas = 735 + 15 + 10 + 351.75 + 5726.18 = 6,837.93 V= Orsat Analysis 735 y CO2 = x100% = 10.75% 6,837.93 15 y CO = x100% = 0.22% 6,837.93 10 y NO = x100% = 0.15% 6,837.93 351.75 yO2 = x100% = 5.14% 6,837.93 5726.18 y N2 = x100% = 83.74% 6,837.93 Example No.3 (Unknown Fuel with known Orsat analysis) A gas turbine power plant receives an unknown type of hydrocarbon fuel. Some of the fuel is burned with air, yielding the following Orsat analysis of the products of combustion, CO2 = 10.5%; O2 = 5.3% and N2 = 84.2%. Determine a. the percentage, by mass, of carbon and hydrogen in the fuel b. the percentage of theoretical air. C n H m + aO 2 + a (3.76) N 2 → 10.5CO2 + bH 2 O + 5.3O 2 + 84.2 N 2 By carbon balance 1(n) = 10.5 n = 10.5 By nitr0gen balance a(3.76)2 = 84.2(2) 84.2 a= = 22.394 3.76 Oxygen balance 2(22.394) = 2(10.5) + b + 2(5.3) b = 13.19 By hydrogen balance 1(m) = 2b m = 26.38 Combustion Equation C10.5 H 26.38 + 22.394O 2 + 84.2 N 2 → 10.5CO2 + 13.19H 2 O + 5.3O 2 + 84.2 N 2 12(10.5) = 82.69% 12(10.5) + 1(26.38) 1(26.38) %H = = 17.31% 12(10.5) + 1(26.38) %C = 22.394(32) + 84.2(28) A = = 20.18 12(10.5) + 1(26.38) F Actual 137.2810.5 + 0.25(26.38) A = = 15.4% 12(10.5) + 1(26.38) F T heoretical % Theoretica l air = (100 + 15.4) = 115.4% Example No.4 (Hydrocarbon Fuel) A fuel represented by C7H16 is oxidized with 20% excess air and the mass of fuel required for combustion is 50 kg/hr. Determine the mass flow rate of the products in kg/hr. A 137.28(1.20)(7 + 4) kg of air = = 20.592 F (84 + 4) kg fuel m p = m F (20.592) + m F m p = 50(21.592) = 1079.6 kg/hr Problem: (Hydrocarbon Mixture and DPT) A fuel with a molal analysis of 80% C12H26 and 20% C14H30 is burned with 30% excess air. The flue gas is at atmospheric pressure. Find the minimum exhaust temperature to avoid condensation if P = 101 KPa. Basis 100 moles of fuel Combustion with 100% TA 80C12H 26 + 20C14H 30 + aO 2 + a (3.76) N 2 → bCO2 + cH 2 O + a (3.76) N 2 Carbon Balance 80(12) + 20(14) = b b = 1,240 Hydrogen balsnce 80(26) + 20(30) = 2c c = 1,340 Oxygen balance 2a = 2b + c a = 1,910 Combustion with EA (e = 0.30) 80C12H 26 + 20C14H 30 + (1.30)aO 2 + (1.30)a (3.76) N 2 → bCO2 + cH 2 O + dO 2 + (1.30)a (3.76) N 2 By oxygen balance d = 573 Combustion Equation 80C12H 26 + 20C14H 30 + 2,483O 2 + 9,336.08N 2 → 1,240CO2 + 1,340H 2 O + 573O 2 + 9,336.08N 2 n Pr oducts = 1,240 + 1,340 + 573 + 9,336.08 = 12,489.08 PH 2 O P = n H 2O n Pr oducts 1,340 = 10.84 KPa 12,489.08 at 10.84 KPa = 47.417C PH 2 O = 101 DPT = t sat Problem Natural Gas A natural gas fuel showed the following percentages by volume: C 2H6 = 9%; CH4 = 90%; CO2 = 0.2 % and N2 = 0.8 %. If this gas is used as fuel and is burned with 20% excess air for complete combustion, Determine a) The Combustion Equation b) The theoretical and actual air fuel ratio c) The molecular weight and gas constant of the products d) The volume of air required per m3 of natural gas if the gas and air are at temperature of 16C and a pressure of 101.6 KPa. Combustion with 100% theoretic al air 9C 2 H 6 + 90CH4 + 0.2CO2 + 0.8N 2 + aO 2 + a(3.76)N 2 → bCO2 + cH 2 O + dN 2 Carbon Balance 2(9) + 90 + 0.2 = b b = 108.2 Hydrogen Balance 9(6) + 90(4) = 2c c = 207 Oxygen Balance 2(0.2) + 2a = 2b + c 2(108.2) + 207 - 2(0.2) a= 2 a = 211.5 Nitrogen Balance 2(0.8) + 2(a)(3.76) = 2d 2(0.8) + 2(211.5)(3.76) d= 2 d = 796.04 Combustion with excess air 9C2 H 6 + 90CH4 + 0.2CO2 + 0.8N2 + (1.20)aO2 + (1.20)a(3.76)N2 → bCO2 + cH 2O + eO2 + fN 2 By oxygen balance 2(0.2) + 2(1.20)(211.5) = 2(108.2) + 207 + 2e 2(0.2) + 2(1.20)(211.5) − 2(108.2) − 207 e= 2 e = 42.3 By Nitrogen balance 2(0.8) + 2(1.20)(211.5)(3.76) = 2f 2(0.8) + 2(1.20)(211.5)(3.76) f= 2 f = 955.088 Combustion Equation 9C2 H 6 + 90CH4 + 0.2CO2 + 0.8N2 + 253.8O2 + 954.288N2 → 108.2CO2 + 207H 2O + 42.3O2 + 955.088N2 Mass of Fuel 9(30) + 90(16) + 0.2(44) + 0.8(28) = 1741.2 kg Mass of air 253.8(32) + 954.288(28) = 34841.664 kg 34841.664 kg of air A = = 20.01 1741.2 kg of fuel F actual A A = (1 + e) F actual F theoretical 20.01 kg of air A = = 16.68 kg of fuel F theoretical 1.20 Moles of Products 108.2 + 207 + 42.3 + 955.088 = 1312.588 108.2(44) + 207(18) + 42.3(32) + 955.088(28) yiMi = M = 1312.588 kg M = 27.9 kg mol R= 8.3143 KJ = 0.298 27.9 kg - K PVa = n a RT (253.8 + 954.288)(8.3143)(16 + 273) = 28571.2 m 3 101.6 PVF = n F RT Va = (9 + 90 + .2 + 0.8)(8.143)(16 + 273) = 2365 m 3 101.6 Va 28571.2 = = 12.08 VF 2365 VF = Sample Problem (Unknown Fuel – Known Orsat analysis) An unknown hydrocarbon is used as fuel in a diesel engine, and after an emission test the orsat analysis shows, CO2 = 12.5% ; CO = 0.3% ; O2 = 3.1% ; N2 = 84.1%.Determine a. the actual air-fuel ratio b. the percent excess air c. the fuel analysis by mass CnHm + aO2 + a(3.76)N2 → 12.5CO2 + bH2O + 0.3CO + 3.1O2 + 84.1N2 By Carbon balance n = 12.5 + 0.3 n = 12.8 By Hydrogen balance m = 2b → eq. 1 By Oxygen balance 2a = 2(12.5) + b + 0.3 + 2(3.1) → eq. 2 By Nitrogen balance a(3.76) = 84.1 a = 22.367 substituting a to eq. 2 b = 13.234 substituting b to eq. 1 m = 26.47 C12.8H 26.47 + 22.367O 2 + 84.1N 2 → 12.5CO2 + 13.234H 2O + 0.3CO + 3.1O2 + 84.1N 2 22.367(32) + 84.1(28) kg of air A = 17.05 = 12(12.8) + 26.47 kg of fuel F a Combustion with 100% theoretical air n = 12.8 ; m = 26.47 C12.8 H 26.47 + aO 2 + a (3.76) N 2 → bCO2 + cH 2 O + a (3.76) N 2 12.8 = b 26.47 = 2c c = 13.235 2a = 2b + c a = 19.4175 kg of air A 19.4175(32) + 19.4175(3.76)( 28 = 14.8 = 12(12.8) + 26.47 kg of C12H 26 F t A A = (1 + e) F a F t e = 0.152 = 15.2 % 12n 12(12.8) = = 85.3% 12n + m 12(12.8) + 26.47 m 26.47 %H = = = 14.7% 12n + m 12(12.8) + 26.47 %C = Properties of Fuels and Lubricants a) Viscosity - a measure of the resistance to flow that a lubricant offers when it is subjected to shear stress. b) Absolute Viscosity - viscosity which is determined by direct measurement of shear resistance. c) Kinematics Viscosity - the ratio of the absolute viscosity to the density d) Viscosity Index - the rate at which viscosity changes with temperature. e) Flash Point - the temperature at which the vapor above a volatile liquid forms a combustible mixture with air. f) Fire Point - The temperature at which oil gives off vapor that burns continuously when ignited. g) Pour Point - the lowest temperature at which a liquid will continue to flow h) Dropping Point - the temperature at which grease melts. i) Condradson Number(carbon residue) - the percentage amount by mass of the carbonaceous residue remaining after destructive distillation. j) Octane Number - a number that provides a measure of the ability of a fuel to resist knocking when it is burnt in a gasoline engine. It is the percentage by volume of iso-octane in a blend with normal heptane that matches the knocking behavior of the fuel. k) Cetane Number - a number that provides a measure of the ignition characteristics of a diesel fuel when it is burnt in a standard diesel engine. It is the percentage of cetane in the standard fuel. ENTHALPY OF FORMATION The “Enthalpy of Formation of a compound is the enthalpy at the Arbitrary Reference State (t = 25C and P = 1 Atm). 1 mole C 25C, 1 atm Combustion Chamber 1 mole CO2 25C, 1 atm 1 mole O2 25C, 1 atm Q Let; HR – total enthalpy of Reactants HP – total enthalpy of products From 1st Law Q + HR = HP or Q + Σ ni hi = Σ ni hi R P but the enthalpy of all the reactants is Zero (for they are all elements) Q = H P = -393,757 KJ therefore (h f ) CO 2 = −393,757 KJ → Enthalpy of formation of CO2 kg m Note : Negative sign is due to the reaction' s being " Exothermic " FIRST LAW ANALYSIS FOR STEADY STATE REACTING SYSTEM W 1 mole C 25C, 1 atm Combustion Chamber 1 mole CO2 25C, 1 atm 1 mole O2 25C, 1 atm By energy balance Q Q + Σ ni hi = W + Σ ni hi R P In most cases, neither the reactants nor the products are at the reference state (t = 25C and P = 1 Atm). In these case we must account for the property change between the reference state and the actual state. The change in enthalpy between the reference state and the actual state is (h − h 298 ) where − denotes that the pressure is 1 Atmosphere General Equation for a Steady State, Steady flow reaction process Q + Σ n i h f + (h − h298) i = W + Σ n j h f + (h − h298) R P j ADIABATIC FLAME TEMPERATURE 1 mole C 25C, 1 atm Combustion Chamber 1 mole CO2 25C, 1 atm 1 mole O2 25C, 1 atm If Q = 0 ; W = 0 ; KE = 0 and PE = 0, all the thermal energy would go into raising the temperature of the products of combustion. When the combustion is complete, the maximum amount of chemical energy has been converted into thermal energy and the temperature of the product is at its maximum. This maximum temperature is called the “ Adiabatic Flame Temperature” (AFT) HR = HP ENTHALPY OF COMBUSTION OR HEATING VALUE It is the difference between the enthalpies of the products and the reactants at the same temperature T and Pressure P. h RP = H P − H R KJ kg mol h RP = Σ n j h f + (h − h298) − Σn i h f + (h − h298) P i KJ kg mol (H P − H R ) KJ M kg where M - molecular weight h RP = HEATING VALUE FORMULAS Heating Value - is the energy released by fuel when it is completely burned and the products of combustion are cooled to the original fuel temperature. Higher Heating Value (HHV) - is the heating value obtained when the water in the products is liquid. Lower Heating Value (LHV) - is the heating value obtained when the water in the products is vapor. For Solid Fuels O KJ HHV = 33,820C + 144,212 H2 − 2 + 9,304S 8 kg where: C, H2, O2, and S are in decimals from the ultimate analysis on an ashless basis For Coal and Oils with the absence of Ultimate Analysis HHV A kg of air/kg of fuel = F t 3,041 HHV = 31,405C + 141 647H KJ/kg For Liquid Fuels HHV = 43,385 + 93(Be - 10) KJ/kg Be - degrees Baume For Gasoline HHV = 41,160 + 93 (API) KJ/kg LHV = 38,639 + 93 (API) KJ/kg For Kerosene HHV = 41,943 + 93 (API) KJ/kg LHV = 39,035 + 93 (API) KJKkg For Fuel Oils HHV = 41,130 + 139.6(API) KJ/kg LHV = 38,105 + 139.6(API) KJ/kg API - American Petroleum Institute For Fuel Oils (From Bureau of Standard Formula) HHV = 51,716 - 8793.8 (S)2 KJ/kg LHV = HHV - QL KJ/kg QL = 2,442.7(9H2) KJ/kg H2 = 0.26 - 0.15(S) kg of H2/ kg of fuel 141.5 131.5+ API 140 S= 130+ Be S= Where: S @ t = S - 0.0007(t-15.56) S - specific gravity of fuel oil at 15.56 C H2 - hydrogen content of fuel oil, Kg H/Kg fuel QL - heat required to evaporate and superheat the water vapor formed by the combustion of hydrogen in the fuel,KJ/kg S @ t - specific gravity of fuel oil at any temperature t Oxygen Bomb Calorimeter - instrument used in measuring heating value of solid and liquid fuels. Gas Calorimeter - instrument used for measuring heating value of gaseous fuels. Sample Problem No. 1 (Coal Fuel/Heating Value) A sample of coal fuel has the following ultimate analysis, percent by mass:H2 = 5.6% ; C = 53.4% ; S = 0.1% ; N2 = 0.1% ; O2 = 37.9% and Ash = 2.9%. This coal will be used as a fuel by burning it with no excess air in a furnace. Determine a) the air--fuel ratio on a mass basis b) the molar analysis of products of combustion c) the HHV of the fuel in KJ/kg O KJ HHV = 33,820C + 144,212 H2 − 2 + 9,304S 8 kg Converting the given U.A. to an ashless basis C = 55% = 0.55 H 2 = 5.8% = 0.058 O 2 = 39% = 0.39 N 2 = 0.103% = 0.00103 S = 0.103% = 0.00103 O kg of air A = 11.44C + 34.32 H 2 − 2 + 4.29S F 8 kg of fuel t A = 6.6 F t O KJ HHV = 33,820C + 144,212 H 2 − 2 + 9,304S 8 kg KJ HHV = 19,889.8 kg SAMPLE PROBLEM NO. 2 A small gas turbine uses C8H18 (liquid) for fuel and 400% theoretical air. The air and fuel enters at 25C and the products of combustion leave at 900 K. The output of the engine and the fuel consumption are measured and it is found that the specific fuel consumption is 0.25 kg/sec of fuel per Megawatt output. Determine the heat transfer from the engine per kgmol of fuel. Assume complete combustion. Q + Σ n i h f + (h − h 298) i = W + Σ n j h f + (h − h 298 ) R P Combustion with 100% TA C8H18 + 12 .5O 2 + 47 N 2 → 8CO 2 + 9H 2O + 47 N 2 Combustion with 400% theoretical air or e = 300% C8H18 + 50 O 2 + 188 N 2 → 8CO 2 + 9H 2O + 37 .5O 2 + 188 N 2 j Q + Σ n i h f + (h − h298) i = W + Σ n j h f + (h − h298) R W= P j 1000 kg KJ 114 = 456,000 0.25 kgm kgm Q + HR = 456,000 + HP KJ Q = −52,776 kg mFuel Q = −463 KJ kg Fuel SAMPLE PROBLEM NO. 3 A diesel engine used gaseous Dodecane (C12H26) as fuel. The air and fuel enters the engine at 25C and 100% excess air is required for combustion. The products of combustion leaves at 600 K and the heat loss from the engine is 232,000 KJ/kgm fuel. Determine the work for a fuel rate of 1 kgm/hr of fuel. Products Air and Fuel W Engine Q = -232,000 KJ/kgmol Q + Σ n i h f + (h − h298) i = W + Σ n j h f + (h − h298) R P j Combustion with 100% theoretical air C12H26 + 18.5O2 + 69.56N2 → 12CO2 + 13H2O + 69.56N2 Combustion with 400% theoretical air or e = 300% C12H26 + 37O 2 + 139.12N2 → 12CO2 + 13H2O + 18.5O 2 + 139.12N2 Q + HR = W + HP W = Q − (HP − HR ) W = −232,000 − (−5,880,284.58) = KJ W = 5,648,284.58 kg mol Fuel 1 W = 5,648,284.58 = 1568.97 KW 3600 SAMPLE PROBLEM No. 4 A fuel oil represented by C10H22 is burned with 25% excess air in a laboratory to determine its heating value. Air and fuel enters at 25C and the products of combustion leaves the apparatus at 500 K. Determine the higher heating value of the fuel considering;(assume hf(C10H22) = -289,402 KJ/kgmol Fuel a) Complete combustion with no CO in the products b) Incomplete combustion with 5% of the carbon atoms oxidizes to CO Combustion with 100% TA C10H 22 + 15.5O 2 + 58.28N 2 → 10CO2 + 11H 2 O + 58.28N 2 Combustion with EA (e = 0.25) C10H 22 + 19.375O 2 + 72.85N 2 → 10CO2 + 11H 2 O + 3.875O 2 + 72.85N 2 Incomplete Combustion Combustion with 125% theoretical air and CO in the products C10H 22 + 19 .063 O 2 + 71 .675 N 2 → 9.5CO 2 + 0.5CO + 11H 2O + 3.813 O 2 + 71 .675 N 2 CHIMNEY By. ENGR. YURI G. MELLIZA FUNCTIONS OF CHIMNEY 1) To dispose the exhaust gases at suitable height so that no pollution will occur in the vicinity. 2) To produce the necessary draft required for the flow of gases. DRAFT - is the difference between the absolute gas pressure at any point in a gas flow passage,(furnace, chimney, air heater and etc.) and the ambient atmospheric pressure. Draft is positive if Pa Pgas and is negative if Pa Pgas. D - diameter of chimney, m H - height of chimney, m THEORETICAL DRAFT(Dt): Dt = 1000H( air − gas ) w ater where: Dt - theoretical draft in mm of water H - height of chimney or smokestack in meters a - density of air in kg/m3 g - density of flue gas in kg/m3 w - density of gage fluid (water) in kg/m3 ACTUAL DRAFT(Da): Da = Dt - DL mm of H2O where: DL - draft losses, and usually expressible in percentage of the theoretical draft. THEORETICAL VELOCITY(v): v = 2ghgas where: v - theoretical velocity of the flue gas in the chimney, m/sec hg - draft in meters of flue gas h gas = D t ( w ater ) m of Gas 1000( gas ) ACTUAL VELOCITY OF FLUE GAS(v'): v' = kv where: K - velocity coefficient, whose value ranges from 0.30 to 0.50 DIAMETER OF CHIMNEY(D): D= 4Q gas v' where: Qg - volume flow rate of flue gas, m3/sec VOLUME FLOW RATE OF FLUE GAS Q gas mgas m3 = gas sec mg = mass flow rate of flue gas, kg/sec MASS FLOW RATE OF FLUE GAS: a) Without considering Ash loss: A m gas = mFuel + 1 F b) Considering Ash loss A mgas = mFuel + 1 − Ash Loss F Where: Ash loss in decimal VOLUME FLOW RATE OF PRODUCTS OF COMBUSTION (Obtained from the balanced combustion equation) PV = nRT n + nH2O + n SO 2 + n O 2 + nN2 + n CO + n CH + nNO + nNO2 + nNO3 n = CO2 kg Fuel nRT kg m 3 V= mFuel P sec sec Q gas = V in m 3/ sec MOLECULAR WEIGHT and GAS CONSTANT OF PRODUCTS OF COMBUSTION Mass of Products Total Moles of Products nCO2MCO2 + nH2OMH2O + nSO2MSO2 + nO2MO2 + nN2MN2 + nCOMCO + nCHMCH + nNOMNO + nNO2MNO2 + nNO3MNO3 M= nPr oducts M= R= R KJ M kg − K Problem No. 1 A power plant at an elevation 0f 600 m has a chimney with an actual draft of 19 mm of H 2O and frictional losses of 15%. Flue gases at the rate of 5 kg/sec enters the chimney at 180C and leaves the chimney at 150C, with a volumetric analysis of CO2 = 12.7% H2O = 2.2% SO2 = 0.1% O2 = 6.8% N2 =77.9% CO = 0.30% and leaves the chimney at 150C. Calculate the height and diameter of the chimney assuming velocity coefficient of k = 0.40. (Ps = 760 mm Hg and Ts = 294 K) ANSWER: H = 98.6 M ; D = 1.3 m M = ΣyiMi M Flue Gas = 12.7(44) + 2.2(18) + 0.1(64) + 6.8(32) + 77.9(28) + 0.30(28) M Flue Gas = 30.12 R Flue Gas = 8.3143 KJ = 0.276 30.12 kg - K At 600 m elevation and standard atmosphere P600 m = 94.44 KPa T600 m = 290.1 K ρ air = P kg = 1.134 3 RT m 180 + 150 = + 273 = 438K 2 94.44 kg ρ Gas = = 0.781 3 (0.276)( 438) m D a = D t − 0.15D t TGas ave 19 = 22.353 mm H 2 O (1 − 0.15) 1000H(ρ air − ρ Gas ) Dt = mm H 2 O ρ water Dt = ρ water = 1000 H = 63.32 m kg m3 4Q gas D= πv' v' = kv v = 2gh gas h gas = D t (ρ water ) m of Gas 1000(ρ gas ) h gas = 28.62 m of flue gas v = 23.70 m sec v' = 0.40(23.70) = 9.48 Qgas = 5 ρ gas = 6.4 m sec m3 sec D = 1.5 m Problem No. 2 A steam power plant using high grade coal having the Ultimate analysis as follows, C = 81% ; H 2 = 12.0% ; O2 = 1.2%; N2 = 1.6% ; S = 2.4%; H2O = 1.7% and Ash = 0.1% requires 30% excess air for complete combustion. Exhaust gases in the smokestack has an average temperature of 650K and pressure of 109 KPaa and produces and actual draft of 27 mm of water with average draft losses of 11% and coefficient k in the stack of 0.35. Ambient air condition is 101 KPa and 25C. For a coal consumption of 1500 kg/hour as fired, determine the required height and diameter of the smokestack. Ultimate Analysis C = 81% H 2 = 12% O 2 = 1.2% N 2 = 1.6% S = 2.4% H 2 O = 1.7% A = 0.1% Comp. C H2 O2 N2 S H2O Ash Denominator UA 81 12 1.2 1.6 2.4 1.7 0.1 (100-0.10 Ashless(xi) 81.1 12.01 1.201 1.602 2.402 1.702 100 Mi 12 2 32 28 32 18 - Xi/Mi 0.068 0.06 0.0004 0.0006 0.0008 0.0009 0.1303 Yi(Molal) 51.87 46.1 0.29 0.44 0.58 0.73 100 Combustion with 100%TA Basis :100 moles of Fuel 51.87C + 46.1H 2 + 0.29O 2 + 0.44 N 2 + 0.58S + 0.73H 2 O + xO 2 + x (3.76) N 2 → aCO2 + bH 2 O + cSO 2 + dN 2 51.87C + 46.1H 2 + 0.29O 2 + 0.44 N 2 + 0.58S + 0.73H 2 O + 75.21O 2 + 282.78N 2 → 51.87CO2 + 46.83H 2 O + 0.58SO 2 + 283.22 N 2 Combustion with EA(Excess air = 0.30) 51.87C + 46.1H 2 + 0.29O 2 + 0.44 N 2 + 0.58S + 0.73H 2 O + 1.30(75.21)O 2 + 1.30(282.78) N 2 → 51.87CO2 + 46.83H 2 O + 0.58SO 2 + eO 2 + fN 2 51.87C + 46.1H 2 + 0.29O 2 + 0.44 N 2 + 0.58S + 0.73H 2 O + 97.77O 2 + 367.61N 2 → 51.87CO2 + 46.83H 2 O + 0.58SO 2 + 22.56O 2 + 368.05N 2 n Pr oducts = 489.89 n Pr oducts (8.3143)(650) = 24,288.86m 3 109 Mass of Fuel = 767.63 kg VPr oducts = m 3 of Products = 31.64 kg of Fuel VF Pr oducts = 31.64(1500) = 47,462.07 VF Pr oducts = 13.18 m 3 of Products hr m 3 of Products sec Da = Dt - DL mm of H2O 27 = D t − 0.11D t Dt = 27 = 30.34 mm H 2 O 1 − 0.11 h gas = D t (ρ water ) m of Gas 1000(ρ gas ) ρ gas = P R g Tg M g = ΣyiMi = Σmi ng 51.87(44) + 46.83(18) + 0.58(64) + 22.56(32) + 368.05(28) = 28.96 51.87 + 46.83 + 0.58 + 22.56 + 368.05 Rg = 0.287 P kg ρ gas = = 0.58 3 R g Tg m Mg = 101 kg = 1.18 3 0.287(25 + 273) m 30.34(1000) = m of Gas 1000(0.58) = 51.92 m of gas ρ air = h gas h gas v = 2gh g = 31.92 m sec v' = kv = 0.35(31.92) = 11.17 Dt = H= 1000H(ρ air − ρ Gas ) mm H 2 O ρ water D t ρ water = 50.93 m 1000(ρ air − ρ Gas ) Qg = D= m sec πD 2 ( v' ) 4 4Q g π ( v' ) = 1.23 m Problem no. 3 The actual velocity of a gas entering in a chimney is 8 m/sec. the gas temperature is 25C and pressure of 98 KPa with a gas constant of 0.287 KJ.kg-K. Determine the chimney diameter if mass of gas is 50,000 kg/hr. (1.37 m) COMBUSTION ENGINEERING QUIZ NO. 1(April 15, 2019) Name _______________________ Problem No. 1 A fuel represented by C7H16 is oxidized with 20% excess air and the mass of fuel required for combustion is 50 kg/hr. Determine the mass flow rate of the products in kg/hr. Fuel : C 7 H16 e : 20% kg hr Combustion with 100% TA C 7 H16 + aO 2 + a(3.76)N2 → bCO2 + cH 2 O + a(3.76)N2 m Fuel : 50 a = n + 0.25m = 11 b=n=7 c = 0.5m = 8 Combustion with EA (e = 0.20) C 7 H16 + (1.20)aO 2 + (1.20)a(3.76)N2 → bCO2 + cH 2 O + dO 2 + (1.20)a(3.76)N2 d = e(n + 0.25m) = 2.2 Combustion Equation C 7 H16 + 13O 2 + 49.632N 2 → 7CO2 + 8H 2 O + 2.2O 2 + 49.632N 2 Mass of Products (m products) m products = 7(44) + 8(18) + 2.2(32) + 49.632(28) = 1,912.10 kg Mass of Products per kg of fuel m products 1,912.10 1,912.10 kg Products = = = 19.12 m Fuel 12(7) + 16 100 kgFuel M Pr oducts − mass flow rate of products M Products = 19.12(50) = 956 kg hr Problem No. 2 The analysis of the natural gas showed the following percentages by volume: C2H6 = 9%; CH4 = 90%; CO2 = 0.2 % and N2 = 0.8 %. Find the volume of air required per cu,m. of gas if the gas and air are at temperature of 16C and a pressure of 101.6 KPa. Combustion with 100% TA (Basis :100 moles of fuel) 9C 2 H 6 + 90CH4 + 0.2CO2 + 0.8N 2 + aO 2 + a (3.76) N 2 → bCO2 + cH 2 O + dN 2 Carbon Balance 2(9) + 90 + 0.2 = b b = 108.2 Hydrogen Balance 6(9) + 4(90) = 2c c = 207 Oxygen Balance 0.2(2) + 2a) = 2b + c a = 211.5 Nitrogen Balance 2(0.8) + a(3.76)2 = 2d d = 796.04 9C 2 H 6 + 90CH4 + 0.2CO2 + 0.8N 2 + 211.5O 2 + 795.24 N 2 → 108.2CO2 + 207H 2 O + 796.04 N 2 n Air = 211.5+ = 795.24 = 1,006.74 Moles n Gas = 100 PV = n RT n RT P At the same temperaru te and pressure, the mole ratio is equal to volumetri c ratio V= m 3 of Air 1,006.74 = = 10.06 100 m 3 of fuel Problem No. 3 A fuel with a molal analysis of 80% C12H26 and 20% C14H30 is burned with 30% excess air. The flue gas is at P = 101 KPa. Dtermine a. the combustion equation b. the actual air-fuel ratio c. the partial of H2O and DPT in the products Combustion with 100% TA (basis; 100 moles of fuel) 80C12H 26 + 20 C14H 30 + aO 2 + a(3.76)N 2 → bCO2 + cH 2 O + a(3.76)N 2 80(12) + 20(14) = b b = 1240 80(26) + 20(30) = 2c c = 1340 2a = 2b + c a = 1910 Combustion with EA (e = 0.30) 80C12H 26 + 20 C14H 30 + (1.30)aO 2 + (1.30)a(3.76)N2 → bCO2 + cH 2 O + dO 2 + (1.30)a(3.76)N2 1.30a (2) = b(2) + c + 2d d = 573 Combustion Equation 80C12H 26 + 20 C14H 30 + 2483O 2 + 9336.08N 2 → 1240CO2 + 1340H 2 O + 573O 2 + 9336.08N 2 2483(32) + 9336.08(28) A = 19.41 Actual = 80(170) + 20(198) F n Pr oducts = 1240 + 1340 + 573 + 9336.08 = 12,489.08 PH2O 1340 = P 12,489.08 PH2O 1340 = 101 12,489.08 PH2O = 10.84 KPa DPT = tsat at 10.84 KPa DPT = 47.417C COMBUSTION ENGINEERING QUIZ NO. 2 (April 23, 2019) Name ______________________________ Problem No. 1 The mass analysis of hydrocarbon fuel A is 88.5% Carbon and 11.5% Hydrogen. Another hydrocarbon fuel B requires 6% more air than fuel A for complete combustion. Calculate the mass analysis of Fuel B. For Fuel A A = 11.44(0.885) + 34.32(0.115) = 14.07 F For Fuel B A = (1.06)(14.07) = 14.915 F C + H =1 C = (1 − H) A = 11.44(1 − H) + 34.32H = 14.915 F 14.915 − 11.44 = (34.32 − 11.44)H H = 0.1519 = 15.19% C = (1 − .1519) = 0.8481 = 84.81% Problem No. 2 A diesel engine uses a hydrocarbon fuel represented by C12H26 and is burned with 30% excess air. The air and fuel is supplied at 1 atm and 25C. Determine a. the actual air-fuel Ratio b. the m3 of CO2 formed per kg of fuel if the product temp. is 400C and a pressure of 1 atm. c. The M and R of the Products d. The M and R of the dry flue gas e. If 1.5 moles of carbon oxidizes to CO, determine the molecular weight of the resulting products Combustion with 130%TA C12H 26 + (1.30)aO 2 + (1.30)a(3.76)N 2 → bCO2 + cH 2 O + dO 2 + (1.30)a(3.76)N 2 b=n b = 12 a = n + 0.25m = 18.5 c = 0.5m = 13 d = e(n + 0.25m) = 5.55 C12H 26 + 24.05O 2 + 90.428N 2 → 12CO2 + 13H 2 O + 5.55O 2 + 90.428N 2 (1.30)137.28(n + 0.25m) A = = 19.42 F 12m + m Actual 12(8.3143)(400 + 273) VCO 2 = = 662.7 m 3 101.325 VCO 2 662.7 = = 3.9 m Fuel 12(12) + 26 n Pr oducts = 12 + 13 + 5.55 + 90.428 = 120.98 M= m Pr oducts 12(44) + 13(18) + 5.55(32) + 90.428(28) kg = = 28.7 n Pr oducts 120.98 kg mol 8.3143 KJ = 0.29 28.7 kg - K m Dry flue gas = 12(44) + 5.55(32) + 90.428(28) = 104.09 R= M Dry Flue Gas = 12 + 5.55 + 90.428 kg = 29.82 104.09 kg mol Combustion with CO and with 100%TA C12 H 26 + aO 2 + a(3.76)N 2 → bCO2 + cH 2 O + 1.5CO + a(3.76)N 2 12 = b + 1.5 b = 12 - 1.5 = 10.5 26 = 2c c = 13 2a = 2b + c + 1.5 c 1.5 a = b+ + = 17.75 2 2 Combustion with CO and with EA (e = 0.30) C12 H 26 + (1.30)aO 2 + (1.30)a(3.76)N 2 → bCO2 + cH 2 O + 1.5CO + dO 2 + (1.30)a(3.76)N 2 By oxygen balance d = 5.325 C12 H 26 + 23.075O 2 + 86.762N 2 → 10.5CO 2 + 13H 2 O + 1.5CO + 5.325O 2 + 86.762N 2 n Pr oducts = 10.5 + 13 + 1.5 + 5.325 + 86.762 = 117.09 M= 10.5(44) + 13(18) + 1.5(28) + 5.325(32) + 86.762(28) kg = 28.51 117.09 kg mol COMBUSTION ENGINEERING QUIZ NO. 3 (April 24, 2019) Name ___________________________________ Problem 1: Calculate the theoretical oxygen and air required to burn 1 kgmol of carbon, and 1 kgmol of Hydrogen. H 2 + 1 O 2 → H 2O 2 C + O 2 → CO 2 2 + 16 → 18 12 + 32 → 44 3 + 8 → 11 kgO 2 8 = = 2.67 kgC 3 kgAir = 11.44 kgC 1+ 8 → 9 kgO 2 8 = =8 KgH 1 kgAir = 34.32 KgH Problem 2: Calculate the theoretical Oxygen--fuel ratio and Air--fuel ratio on a mass basis for the combustion of ethanol, C2H5OH. Combustion with 100% TA C 2 H 5OH + aO 2 + a (3.76) N 2 → bCO2 + cH 2 O + a (3.76) N 2 2=b 5 + 1 = 2c c=3 1 + 2a = 2b + c 2(2) + 3 − 1 a= =3 2 C 2 H 5OH + 3O 2 + 11.28N 2 → 2CO2 + 3H 2 O + 11.28N 2 kgOxygen 3(32) 96 = = kgFuel 124 + 5 + 16 + 1 46 kgAir 3(32) + 11.28(28) = = kgFuel 124 + 5 + 16 + 1 Problem 3: Determine the molal analysis of the products of combustion when octane C8H18 is burned with 100% excess air. Combustion with EA (e = 100%) C8 H18 + (1 + 1)aO 2 + (1 + 1)a (3.76) N 2 → bCO2 + cH 2 O + dO 2 + (1 + 1)a (3.76) N 2 a = n + 0.25m b=n c = 0,5m d = e(n + 0.25m) C8 H18 + 24.5O 2 + 92.12 N 2 → bCO2 + cH 2 O + dO 2 + (1 + 1)a (3.76) N 2 C8 H18 + 25O 2 + 94 N 2 → 8CO2 + 9H 2 O + 12.5O 2 + 94 N 2 n Pr oducts = 8 + 9 + 12.5 + 94 = 123.5 8 y CO 2 = x100% = 6.48% 123.5 9 y H 2O = x100% = 7.29% 123.5 12.5 y O2 = x100% = 10.12% 123.5 94 y N2 = x100% = 76.11% 123.5 Problem 4: A certain fuel has the composition C10H22. If this fuel is burned with 50% excess air, what is the composition of the products of combustion? Combustion with EA (e = 50%) C10H 22 + 23.25O 2 + 87.42 N 2 → 10CO2 + 11H 2 O + 7.75O 2 + 87.42N 2 a = n + 0.25m b=n c = 0,5m d = e(n + 0.25m) Problem 5: A sample of pine bark has the following ultimate analysis, percent by mass: C = 53.4% ; H 2 = 5.6% ; O2 = 37.9% ; N2 = 0.1% ; S = 0.1% ; Ash = 2.9%. This bark will be used as a fuel by burning it 30% excess air. Determine the actual air-fuel ratio. Fuel UA Ashless C H2 O2 N2 S H20 Ash Total 53.4 5.6 37.9 0.1 0.1 0 2.9 100 55 5.8 39 0.103 0.103 0 0 100 O A = 11.44C + 34.32 H 2 − 2 + 4.29S = 6.6 8 F T heoretical A A = (1 + e) = 8.58 F Actual F T heoretical COMBUSTION ENGINEERING Activity No. 4 (APRIL 29, 2019) NAME __________________________________ Problem No. 1 A combustor receives 340 m3/min of natural gas having a volumetric chemical composition of 15% C2H6 and 85% CH4 that requires 25% excess air. Air and fuel enters the combustor at 25C (298 K)and 101 KPa and products of combustion leaves at 1100 K. Emission test gives that 2 moles of CO and 1 mole NO is found in the products. Determine a. The actual combustion equation b. The actual air – fuel ratio c. The heating value of the fuel (HP – HR) KJ/kg d. The mass flow rate of fuel in kg/min e. The volume flow rate of emission gases (CO2, CO and NO) in m3/hr C2H6: M = 30; Cp = 1.7549 KJ/kg-K; Cv = 1.4782 KJ/kg-K CH4: M = 16; Cp = 2.1377 KJ/kg-K; Cv = 1.6187 KJ/kg-K Combustion with 100% TA Basis :100 moles of fuel 15C 2 H 6 + 85CH4 + aO 2 + a(3.76)N 2 → bCO2 + cH 2 O + 2CO + 1NO + dN 2 15C 2 H 6 + 85CH4 + 222O 2 + 834.72N 2 → 113CO2 + 215H 2 O + 2CO + 1NO + 834.22 N 2 Combustion with EXCESS AIR(e = 0.25) Basis :100 moles of fuel 15C 2 H 6 + 85CH4 + (1.25)222O 2 + (1.25)834.72N 2 → 113CO2 + 215H 2 O + 2CO + 1NO + fO 2 + gN 2 15C 2 H 6 + 85CH4 + 227.5O 2 + 1,043.4 N 2 → 113CO2 + 215H 2 O + 2CO + 1NO + 55.5O 2 + 1,042.9 N 2 227.5(32) + 1,043.4(28) A = = 21.05 15(30) + 85(16) F Actual Problem No. 2 Calculate the theoretical air – fuel ratio of the Hydrocarbon Fuel in the table below. Fuel C8H18 C7H16 C4H10 C9H20 C11H24 Theoretical (By Mass) 15.05 15.10 15.38 15.02 14.96 A/F Ratio COMBUSTION ENGINEERING Activity No. 5 (May 02, 2019) NAME __________________________________ A hydrocarbon Fuel C7H16 (n-Heptane) was tested in a laboratory in order to determine its LHV and HHV. The fuel is burned with 50% excess air requirement for complete combustion. Air and fuel enters the apparatus at 25C and 101 KPa, while the products of combustion leaves the apparatus at 600 K. Determine a. the combustion equation b. the LHV in KJ/kg of fuel c. the HHV in KJ/kg of fuel hf of C7H16 = -187,900 KJ/kgm For HHV For LHV COMBUSTION ENGINEERING Activity No. 6 (May 03, 2019) NAME __________________________________ Multiple Choice Instruction: Write the letter, which corresponds to the correct answer in the table below. 1. A hydrocarbon fuel represented by C8H18 is burned with air. Its gas constant in KJ/kg-K is equal to; a. 0.073 b. 0.286 c. 0.0826 d. 0.187 2. A gaseous mixture has the following volumetric analysis O2, 30%; CO2, 40% N2, 30%. Determine its molecular weight in kg/kgmol. a. 25.6 b. 35.6 c. 28.9 d. 30.2 3. The products of combustion of an automotive engine using a diesel fuel has an Orsat analysis as follows; CO 2 = 12.5%; O2 = 3.5%; CO = 0.5%; N2 = 83.5%. The gas constant of the dry flue gas is equal to; a. 0.287 b. 1.0045 c. 0.1889 d. 1.007 4. A newly designed high speed European car uses high grade gasoline fuel represented by C 8H18. If this fuel is burned with 30% excess air, determine the actual air-fuel ratio. a. 20.5 b. 10.87 c. 15.8 d. 19.6 5. A fuel represented by C7H16 is oxidized with 20% excess air and the mass of fuel required for combustion is 50 kg/hr. Determine the mass flow rate of the products in kg/hr. a. 956.05 b. 906.05 c. 806.07 d. 856.07 6. There are 20 kg of flue gas formed per kg of fuel burned for the combustion of C 12H26. What is the percent excess air. a. 27.17 b. 16.56 c. 26.67 d. 8.21 7. For a certain ideal gas mixture, R = 0.270 KJ/kg-k and k = 1.3. Determine the mass of the mixture in kg for 10 moles of the mixture. a. 408 b. 308 c. 508 d. 208 8. Determine the molecular weight of a products if Cp = 1.1 KJ/kg-K and k = 1.3. a. 28.75 b. 26.75 c. 32.75 d.39.75 9. Determine the mass ratio C/H of a hydrocarbon fuel with a chemical formua of C 16H32. a. 8 b. 10 c. 4 d. 6 10. The Dalton’s Law of partial pressure is called the: a. Law of additive volume b. Law of additive mass c. Law of additive moles d. Law of additive pressure Problem: A Fuel Oil belonging to the paraffin family that is 85%C and 15%H is burned in an internal combustion engine and requires 20% excess for complete combustion. Determine; 11) The fuel chemical formula a. C17H36 b. C12H26 c. C10H22 d. C14H30 12) The actual air-fuel ratio a. 14.25 b. 17.85 c. 19.26 d. 20.26 13) The kg of CO2 formed per kg of fuel a. 2.118 b. 1.117 c. 3.117 d. 4.118 14) The partial pressure of H2O if the total pressure of the products is 101 KPa a. 18.72 b. 10.93 c. 75.23 d. 11.54 15) The gas constant R of the products in KJ/kg-K a. 0.2895 b. 0.3762 c. 0.2004 d. 0.3008 ANSWER TABLE 1 a 2 b 3 a 4 d 5 a 6 7 8 9 10 a b c d d 11 12 13 14 15 a b c d a COMBUSTION ENGINEERING MIDTERM EXAM Name ______________________________ Problem A medium size internal combustion engine power plant is situated at an altitude of 800 m above sea level. The engine is 4 – stroke diesel engine using C16H34 with 50% excess air required for combustion. The plant produces 1.5 MW of electrical energy with a specific fuel consumption of 0.30 kg/KW – hr. Sea level condition is P = 760 mm Hg and T = 293 K. Design the required Height and diameter of the smoke stack in the plant with an actual draft of 25 mm of H 2O and assume 10% losses and average flue gas temperature of 350C . Diameter Generator Output = 1,500 KW Height Fuel and air Diesel Engine At 800 m above sea level P = 92.21 KPa T = 287.8 K P kg ρ air = = 1.12 3 RT m Combustion of C16H 34 with 50% excess air C16H 34 + 36.75O 2 + 138.18N 2 → 16CO2 + 17H 2 O + 12.25O 2 + 138.18N 2 16(44) + 17(18) + 12.25(32) + 138.18(28) kg = 28.74 16 + 17 + 12.25 + 138.18 kgm 8.3143 KJ R Pr oducts = = 0.289 M kg - K 183.43(8.3143)(350 + 273) VPr oducts = = 10,304.005 m 3 92.21 3 10,304.005 (0.30)(1500) hr = 5.7 m Q Pr oducts = 12(16) + 34 3600 sec sec M Pr oducts = 92.21 kg = 0.51 3 (0.289)(350 + 273) m D a = D t − 0.10D t = 25 mm water ρ Pr oducts = D t = 28.09 mm 28.09(1000) = 54.85 m of flue gas 1000(0.51) m v = 2gh g = 32.80 sec 1000H ρ air - ρ gas Dt = mm water ρ water hg = ( ) H = 46.05 m May 08, 2019 BLOWERS Qg = π 2 D (kv) 4 D= 4(5.7) = 0.7 m π(0.40)(32.80) Blower is a machine used to compressed air or gas by centrifugal force to a final pressure not exceeding 241 KPa gage. Usually blower has no cooling system or it is not water cooled. COMPRESSION OF GASES The design of blower is usually based upon either an adiabatic or isothermal compression. A. Isothermal Compression (PV = C) or (T1 = T2 = T) W (Work/Power of Blower P P2 T2 P1 T1 P2 m m P1V1 = P2 V2 1 V P W = P1V1 ln 2 P1 V1 = Q WBlower = P1Q ln W = − VdP PV = C P1 T1 = T2 2 P2 P1 P1Q = mRT W = QγH H − Isothermal Head ρg 1000 P ρ= RT Pg γ= (1000)RT γ= P2 P1g H = Q P1 (1000)RT1 (1000)RT1 P2 ln meters H= P g 1 P1Q ln B. Isentropic Compression (PVk = C; 0r S = C) P1V1k = P2 V2 k T2 P2 = T1 P1 Q=0 k −1 k W = Q − Δh − ΔKE − ΔPE W = − VdP −ΔKE − ΔPE For a compressor work is done on the system; let - W = Wc Wc − Ideal compressio n work/Po wer in blower − W = WC = Δh − Q + ΔKE + ΔPE k −1 kP1V1 P2 k Wc = − 1 + ΔKE + ΔPE k − 1 P1 If ΔKE & ΔPE are negligible − W = WC = VdP + ΔKE + ΔPE k −1 kP1V1 P2 k VdP = − 1 KW k − 1 P1 k −1 kP1V1 P2 k Wc = − 1 k − 1 P1 P1V1 = mRT1 v 2 2 − v12 KW 2(1000) mg (z 2 − z1 ) ΔPE = KW 1000 ΔKE = Q=0 k −1 kP1V1 P2 k − 1 = QγH Wc = k − 1 P1 V1 = Q γ= P1g (1000)RT1 P1g k −1 kP1Q P2 k EFFICIENCY A. Adiabatic Efficiency ek = Isentropic Work x 100% Brake or Shaft Work B.Isothermal efficiency eIso = Isothermal Work x 100% Brake or Shaft Work C. Brake Power 2πTN KW 60,000 T - Brake Torque inN - m N - n0. of RPM BP = RATIO OF THE ADIABATIC TEMPERATURE RISE TO THE ACTUAL TEMPERATURE RISE K −1 K P 2 T1 − 1 P1 Y= ' T2 − T1 ( ) RELATIONSHIP FOR CORRECTING PERFORMANCE CURVES 1. Volume Flow QB N B = QA N A 2. Weight Flow mB N B P1B T1A = mA N A P1A T1B 3. Pressure Ratio K −1 K P 2 − 1 P1 B N B = K − 1 K NA P2 −1 P1 A P2 = rp (pressure ratio) P1 2 T1A T 1B 4. Head H B N 2B = H A N 2A 5. Brake Power BPB NB = BPA N A 3 P1B P1A T1A T 1B P K −1K 2 − 1 P1 BPB P1B Q B B = BPA P1A Q A P K −1K 2 − 1 P1 A 1 - suction 2 - discharge A - 1st condition B - 2nd condition R - gas constant, KJ/kg-K P - absolute pressure in KPa - density, kg/m3 T - absolute temperature, K - specific weight, KN/m3 Q - capacity, m3/sec BP - brake power, KW N - speed, RPM W - work, KW m - mass flow rate, kg/sec H - head, m Example (Blower) A steam power plant uses coal as fuel having the ultimate analysis as follows: C = 72% ; H2 = 5%; O2 = 10%; N2= 1.2%; S = 3.3%; M = 0.1% & A = 8.4% This coal is burned with 50% excess air for complete combustion. Exhaust gases leaves the boiler at 100 KPa and 600 K and is compressed in a blower isentropically to a pressure of 110 KPa producing the necessary draft in the chimney. If the plant consumes 1.5 MTon per hr of coal, determine the motor power required by the blower for a blower efficiency of 70%. Fuel C H2 O2 N2 S H2O Ash U.A. 72 5 10 1.2 3.3 0.1 8.4 100 Ashless 78.6 5.46 10.92 1.31 3.6 0.11 100 Mi 12 2 32 28 32 18 - Xi/Mi 0.066 0.027 0.003 0.0005 0.0011 0.0001 0.098 Molal Analysis 66.93 27.89 3.49 0.48 1.15 0.06 100 Combustion Equation w ith 50% Excess air 66.93C + 27.89H2 + 3.49O2 + 0.48N2 + 1.15S + 0.06H2O → Fuel 117.81O2 + 442.98N 2 → Air 66.93CO2 + 27.95H 2O + 1.15SO2 + 39.27O 2 + 443.46 N 2 → Pr oducts M Pr oducts = 66.93(44) + 27.95(18) + 1.15(64) + 39.27(32) + 443.46(28) = 29.71 66.93 + 27.95 + 1.15 + 39.27 + 443.46 8.3143 = 0.280 29.71 kg of Products 66.93(44) + 27.95(18) + 1.15(64) + 39.27(32) + 443.46(28) = = 16.83 kg of Fuel 66.93(12) + 27.89(2) + 3.49(32) + 0.48(28) + 1.15(32) + 0.06(18) R= hr kg = 7.011 m Pr oducts = 16.83(1.5)(1000) 3600 sec) sec Products CO2 H2O SO2 O2 N2 n(Moles) 66.93 27.95 1.15 39.27 443.46 Cp = ΣxiCpi = 1.021 Cv = ΣxiCVi = 0.741 Cp k= = 1.378 Cv k −1 kmRT1 P2 k WBlower = − 1 k − 1 P1 P2 = 110 P1=10 0 T1 = 600 K WBlower = 113.7 kw WBlower Brake Power BP = 162.41 KW MP 165 KW e Blower = Mi 44 18 64 32 28 nM(kg) 2,945.10 503.12 73.63 1,256.69 12,416.90 17,195.44 xi 17.13 2.93 0.43 7.31 72.21 100 Cp 0.845 1.866 0.624 0.918 1.041 Cv 0.656 1.404 0.494 0.658 0.744 INTERNAL COMBUSTION ENGINE CYCLE Air Standard Cycle o Otto Cycle o Diesel Cycle o Dual Cycle AIR STANDARD OTTO CYCLE Otto, Nikolaus August Born:June 10, 1832, Holzhausen, Nassau Died: Jan. 26, 1891, Cologne German engineer who developed the four-stroke internal-combustion engine, which offered the first practical alternative to the steam engine as a power source. Otto built his first gasoline-powered engine in 1861. Three years later he formed a partnership with the German industrialist Eugen Langen, and together they developed an improved engine that won a gold medal at the Paris Exposition of 1867. In 1876 Otto built an internal-combustion engine utilizing the four-stroke cycle (four strokes of the piston for each ignition). The four-stroke cycle was patented in 1862 by the French engineer Alphonse Beau de Rochas, but since Otto was the first to build an engine based upon this principle, it is commonly known as the Otto cycle. Because of its reliability, its efficiency, and its relative quietness, Otto's engine was an immediate success. More than 30,000 of them were built during the next 10 years, but in 1886 Otto's patent was revoked when Beau de Rochas' earlier patent was brought to light. Processes 1 to 2 – Isentropic Compression (S = C) 2 to 3 – Constant Volume Heat Addition (V = C) 3 to 4 – Isentropic Expansion (S = C) 4 to 1 – Constant volume Heat Rejection (V = C) Compression Ratio (r) V V r = 1 = 4 →1 V2 V3 V1 = V4 and V2 = V3 V1 - volume at bottom dead center (BDC) V2 – volume at top dead center (TDC)(clearance volume) Displacement Volume (VD) VD =V1 – V2 → Eq. 2 Percent Clearance (C) C= V2 VD r= 1+ C C Heat Added (QA) At V = C ; Q = mCv(T) QA = mCv(T3 – T2) Heat Rejected (QR) QR = mCv(T4 – T1) Net Work (W) W = Q W = Q A – QR P,V and T Relations At point 1 to 2 (S = C) T2 V1 = T1 V2 k −1 = (r )k −1 P = 2 P1 k −1 k P2 = P1 (r ) k V1 r T2 = T1 (r ) k −1 V2 = At point 2 to 3 (V = C) T3 P3 = T2 P2 Q A = mC v (T3 − T2 ) T3 = QA + T2 mC v P3 = P2 T3 T2 At point 3 to 4 (S = C) k −1 P T3 V4 = 3 = T4 V3 P4 P P4 = k3 r T3 = T4 (r ) k −1 k −1 k = (r ) k −1 At point 4 to 1 (V = C) T4 P4 = T1 P1 Entropy Change a) S during Heat Addition T S3 − S2 = mCv ln 3 T2 b) S during Heat Rejection S1 − S4 = mCv T1 T4 Thermal Efficiency e= W x 100% QA e= QA − QR x100% QA Q e = 1 − R x 100% QA (T − T ) e = 1 − 4 1 x 100% (T3 − T2 ) 1 e = 1 − k −1 x 100% (r ) Mean Effective Pressure Pm = W KPa VD VD = V1 − V2 V2 = V1 r 1 VD = V1 1 − r mRT1 1 VD = 1 − P1 r where: Pm – mean effective pressure, KPa W – Net Work KJ, KJ/kg, KW VD – Displacement Volume m3, m3/kg, m3/sec Displacement Volume VD = V1 – V2 m3 → Eq. 20 VD = 1 - 2 m3/kg → Eq.21 Note: For Cold Air Standar: k = 1.4 For Hot Air Standard: k = 1.3 AIR STANDARD DIESEL CYCLE Diesel, Rudolf (Christian Karl) Born: March 18, 1858, Paris, France Died: September 29, 1913, at sea in the English Channel German thermal engineer who invented the internal-combustion engine that bears his name. He was also a distinguished connoisseur of the arts, a linguist, and a social theorist. Diesel, the son of German-born parents, grew up in Paris until the family was deported to England in 1870 following the outbreak of the Franco-German War. From London Diesel was sent to Augsburg, his father's native town, to continue his schooling. There and later at the Technische Hochschule (Technical High School) in Munich he established a brilliant scholastic record in fields of engineering. At Munich he was a protégé of the refrigeration engineer Carl von Linde, whose Paris firm he joined in 1880. Diesel devoted much of his time to the self-imposed task of developing an internal combustion engine that would approach the theoretical efficiency of the Carnot cycle. For a time he experimented with an expansion engine using ammonia. About 1890, in which year he moved to a new post with the Linde firm in Berlin, he conceived the idea for the diesel engine . He obtained a German development patent in 1892 and the following year published a description of his engine under the title Theorie und Konstruktion eines rationellen Wäremotors (Theory and Construction of a Rational Heat Motor). With support from the Maschinenfabrik Augsburg and the Krupp firms, he produced a series of increasingly successful models, culminating in his demonstration in 1897 of a 25-horsepower, four-stroke, single vertical cylinder compression engine. The high efficiency of Diesel's engine, together with its comparative simplicity of design, made it an immediate commercial success, and royalty fees brought great wealth to its inventor. Diesel disappeared from the deck of the mail steamer Dresden en route to London and was assumed to have drowned. Processes: 1 to 2 – Isentropic Compression (S = C) 2 to 3 – Constant Pressure Heat Addition (P = C) 3 to 4 – Isentropic Expansion (S = C) 4 to 1 – Constant Volume Heat Rejection (V = C) Compression Ratio V V r= 1 = 4 V2 V2 V1 V4 V2 V3 Cut-Off Ratio(rc) V3 V2 Percent Clearance V C= 2 VD rc = r= 1+ C C Displacement Volume (VD) VD =V1 – V2 Heat Added (QA) At P = C ; Q = mCp(T) QA = mCp(T3 – T2) QA = mkCv(T3 – T2) Heat Rejected (QR) QR = mCv(T4 – T1) Net Work (W) W = Q W = Q A – QR W = mkCv(T3 – T2) - mCv(T4 – T1) W = mCv[k (T3 – T2) - (T4 – T1)] P,V and T Relations At Point 1 to 2 (S = C) T2 V1 = T1 V2 k −1 = (r ) k −1 P2 = P1r k T2 = T1 (r ) k −1 At Point 2 to 3 (P = C) T3 V3 = = rc T2 V2 Q A = mC p (T3 − T 2) P2 = P1r k P3 = P2 T3 = QA + T2 mCp T3 = T1 (r )k −1 (rc ) υ3 = RT3 P3 rc = υ3 υ2 P = 2 P1 k −1 k At Point 3 to 4 (S = C) T4 V3 = T3 V4 υ1 = υ 4 k −1 P = 4 P3 k −1 k P3 υ 3 k = P4 υ 4 k υ P4 = P3 3 υ4 T4 P4 = T3 P3 P T4 = T3 4 P3 T4 = T1 (r ) T4 = T1 k = 423.4 KPa k −1 k k −1 k −1 k V (rc ) 3 V4 k −1 V1k −1 V3 V3 k −1 V2 k −1 V2 V4 k −1 T4 = T1 (rc ) k At Point 4 to 1 (V = C) T4 P4 = T1 P1 Entropy Change a) S during Heat Addition T S3 − S2 = mCp ln 3 T2 b) S during Heat Rejection T S1 − S4 = mCv ln 1 T4 S1 - S4 = -( S3 – S2) Thermal Efficiency e= W x 100% QA e= QA − QR x 100% QA Q e = 1 − R x 100% QA (T − T ) e = 1 − 4 1 x 100% k (T3 − T2 ) Substituting Eq. 11, Eq. 13 and Eq. 14 to Eq. 22 1 r k − 1 e = 1 − k −1 c x100% (r ) k (rc − 1) Mean Effective Pressure W KPa VD where: Pm – mean effective pressure, KPa W – Net Work KJ, KJ/kg, KW VD – Displacement Volume m3, m3/kg, m3/sec Displacement Volume VD = V1 – V2 m3 → Eq. 25 VD = 1 - 2 m3/kg → Eq.26 Pm = AIR STANDARD DUAL CYCLE Processes: 1 to 2 – Isentropic Compression (S = C) 2 to 3 – Constant Volume Heat Addition Q23 ( V = C) 3 to 4 – Constant Pressure Heat Addition Q34 (P = C) 4 to 5 – Isentropic Expansion (S = C) 5 to 1 - Constant Volume Heat Rejection (V = C) Compression Ratio V1 V2 V1 = V5 and V2 = V3 Cut-Off Ratio r= rc = V4 V3 Pressure Ratio P3 P2 P3 = P4 rp = Percent Clearance C= V2 VD 1+ C C Displacement Volume VD = V 1 – V2 m 3 VD = 1 - 2 r= P, V, and T Relations At point 1 to 2 (S = C) T2 V1 = T1 V2 k −1 = (r ) k −1 P = 2 P1 k −1 k T2 = T1 (r ) k −1 At point 2 to 3 (V = C) T3 P3 = = rP T2 P2 T3 = T1 (r) k −1 (rP ) At point 3 to 4 (P = C) T4 V4 = rc = T3 V3 T4 = T1 (r ) k −1 (rP )(rc ) At point 4 to 5 (S = C) T5 V4 = T4 V5 T5 = T1 k −1 V1k −1 V2 k −1 (r ) V4 V4k−1 k −1 P V2 V1 T5 = T1 (rc ) (rP ) k At 5 to 1 (V = C) T5 P5 = T1 P1 Entropy change a) At 2 to 3 (V = C) S3 − S2 = mC V T3 T2 b) At 3 to 4 (P = C) T4 T3 S4 – S2 = (S3 – S2) + (S4 – S3) S4 − S3 = mCp ln c) At 5 to 1 (V = C) S1 – S5 = mCvln S1 − S5 = mCv T1 T5 Heat Added QA = QA23 + QA34 QA23 = mCv(T3 - T2) QA34 = mCp(T4 - T3) = mkCv(T4 - T3) QA = mCv[(T3 - T2)+ k(T4 - T3) Heat Rejected QR = mCv(T5 - T1) Net Work W = (QA - QR) W = mCv[(T3 - T2) + k(T4 - T3) - (T5 - T1)] Thermal Efficiency e= W x100% QA e= QA − QR x100% QA Q e = 1 − R x 100% QA (T5 − T1 ) e = 1 − x 100% (T3 − T2 ) + k(T4 − T3 ) Substituting rP rc k − 1 1 x100% e = 1 − k −1 (r ) (rP − 1) + krP (rc − 1) SAMPLE PROBLEMS AIR STANDARD CYCLE Example No. 1 An air standard Otto cycle has a compression ratio of 8 and has air conditions at the beginning of compression of 100 KPa and 25C. The heat added is 1400 KJ/kg. Determine: a) the thermal efficiency (56.5%) b) the mean effective pressure (1057 KPa) c) the percent clearance c (14.3%) Given: r = 8; P1 = 100 KPa ; T1 = 298K; QA = 1400 KJ/kg Solution: a. 1 e = 1 − k −1 x 100% (r ) 1 e = 1 − 1.4 −1 x 100% (8) e = 56.5% b) W VD Pm = W = QA − QR e= W QA W = 0.565(1400) KJ W = 791 kg VD = υ1 − υ 2 r= υ1 υ2 υ2 = υ1 r υ1 r 1 VD = υ1 1 − r P1υ1 = RT1 VD = υ1 − m3 1 1 − r = 0.748 kg Pm = 1057 KPa VD = RT1 P1 c) 1+ c c rc = 1 + c c(r − 1) = 1 1 c= = 0.143 = 14.3% r −1 r= Example No. 2 An engine operates on the air standard Otto cycle. The cycle work is 900 KJ/kg, the maximum cycle temperature is 3000C and the temperature at the end of isentropic compression is 600C. Determine the engine's compression ratio and the thermal efficiency.(r = 6.35; e = 52.26%) Given: W = 900 KJ/kg; T3 = 3273K; T2 = 873K QA = Cv(T3 – T2) = 0.7175(3273 – 873) = 1722 KJ/kg e = W/QA e = 52.26% 1 1 k −1 r = 1− e r = 6.36 Example No. 3 An air standard diesel cycle has a compression ratio of 20 and a cut-off ratio of 3. Inlet pressure and temperature are 100 KPa and 27C. Determine: a) the heat added in KJ/kg (1998 KJ/kg) b) the net work in KJ/kg (1178 KJ/kg) c) the thermal efficiency (61%) Given r = 20 rc = 3 P1 = 100KPa T1 = 573K Q A = C p (T3 − T2 ) Rk = 1.0045 k −1 At 1 to 2 (S = C) Cp = T2 = T1 (r )k −1 = 994.3K T3 = rc (T 2) = 2983K Q A = C p (T3 − T2 ) = 1997.65 KJ kg P2 = P1 (r ) k = 6229KPa P2 = P3 At 3 to 4 k −1 υ T4 P4 k = = 3 T3 P3 υ4 RT3 υ3 = = 0.14 P3 k −1 T 4 = 1442.45K Q R = Cv(T4 − T1 ) R = 0.7175 k −1 KJ Q R = 820 kg W = QA − QR = 1167.65 W e= x100% = 59% QA Cv = υ = 3 υ1 k −1 Given: r = 20; rc = 3 Solution: V r= 1 V2 rk = ; P1 = 100 KPa ; T1 = 300C P2 P1 P2 = 100(20)1.4 = 6229 KPa P2 = P3 = 6229 KPa T2 = (r ) k −1 T1 T2 = 300(20)1.4 −1 = 994.3 K T3 V3 = = rc T2 V2 T3 = 994.3(3) = 2983 K υ3 = RT3 0.287(2983) = = 0.14 m 3 P3 6229 υ1 = υ 4 = RT1 0.287(300) = = 0.861 m 3 P1 100 T4 V3 = T3 V4 k −1 1.4 −1 0.14 T4 = 2983 0.861 = 1442.45 K QA = Cp(T3 – T2) = 1.0045(2983 – 994.3) QA = 1997.65 KJ/kg QR = Cv(T4 – T1) = 0.7175(1442.45 – 300) QR = 820 KJ/kg W = QA - QR = (1997.65 – 820) W = 1177.65 KJ/kg e= W x 100% QA 1177.65 x 100% 1997.65 e = 59 % k 1 rc − 1 e = 1 − k −1 ( r ) k ( rc − 1 ) e= ( 3 )1.4 − 1 1 x 100% e = 1 − 1.4 −1 1.4( 3 − 1 ) ( 20 ) e = 60.6 % Example No. 4 An ideal dual combustion cycle operates on 0.454 kg of air. At the beginning of compression air is at 97 KPa, 316K. Let rp = 1.5, rc= 1.6 and r = 11. Determine a. the percent clearance (C = 10%) b. the heat added, heat rejected and the net cycle work c. the thermal efficiency rP rc k − 1 1 x100% e = 1 − k −1 (r − 1) + krP (rc − 1) (r ) P e = 58.7% 1+ C C 1 C= = 10 % r −1 r= QA = Q23 + Q34 Q23 = mCv(T3 – T2) T2 = T1 (r) k −1 = 825 K P2 = P1 (r ) k = 2,784 KPa T3 = T2 (rp ) = 1238 K Q23 = 0.454(0.7175)(1238 – 825) = 135 KJ Q34 = mCp(T4 – T3) T rc = 4 = 1.6 T3 T4 = 1.6T3 T4 = 1981K Q34 = 0.454(1.0045(1981 – 1238) = 339 KJ QA = Q23 + Q34 = 474 KJ Internal Combustion Engine By. ENGR. YURI G. MELLIZA Diesel engine is a type of internal combustion engine that uses low grade fuel oil and which burns this fuel inside the cylinder by heat of compression. It is used chiefly for heavy-duty work. Diesel engines drive huge freight trucks, large buses, tractors, and heavy road-building equipment. They are also used to power submarines and ships, and the generators of electric-power stations in small cities. Some motor cars are powered by diesel engines. Gasoline engine - is a type of internal combustion engine, which uses high grade of oil. It uses electricity and spark plugs to ignite the fuel in the engine's cylinders. Kinds of diesel engines. There are two main types of diesel engines. They differ according to the number of piston strokes required to complete a cycle of air compression, exhaust, and intake of fresh air. A stroke is an up or down movement of a piston. These engines are (1) the four-stroke cycle engine and (2) the two-stroke cycle engine. Four Stroke Cycle Engine 1. Intake 2. Compression 3. Power 4. Exhaust Intake Compression Power Exhaust In a four-stroke engine, each piston moves down, up, down, and up to complete a cycle. The first down stroke draws air into the cylinder. The first upstroke compresses the air. The second down stroke is the power stroke. The second upstroke exhausts the gases produced by combustion. A four-stroke engine requires exhaust and air-intake valves. It completes one cycle in two revolutions of the crankshaft. Two Stroke Cycle Engine 1. Intake-Compression stroke 2. Power-exhaust stroke Intake-compression Power-Exhaust Intake port Exhaust port In a two-stroke engine, the exhaust and intake of fresh air occur through openings in the cylinder near the end of the down stroke, or power stroke. The one upstroke is the compression stroke. A two-stroke engine does not need valves. These engines have twice as many power strokes per cycle as four-stroke engines, and are used where high power is needed in a small engine. It completes one cycle in one revolution of the crankshaft. INTERNAL COMBUSTION ENGINE POWER PLANT Two stroke cycle engine: An engine that completes one cycle in one revolution of the crankshaft. Four stroke cycle engine: An engine that completes one cycle in two revolution of the crankshaft. ENGINE PERFORMANCE 1. 2. HEAT SUPPLIED BY FUEL KJ Qs = m F (HV ) hr where: mf - fuel consumption in kg/hr HV - heating value of fuel in KJ/kg INDICATED POWER P πLD 2 Nn' IP = mi KW 4(60) where: Pmi - indicated mean effective pressure in KPa L - length of stroke in m D - diameter of bore in m n' - no. of cylinders IP - indicated power in KW N = (RPM ) → (For 2 Stroke - Single acting) N = 2(RPM) → (For 2 Stroke - Double acting) (RPM) N= → (For 4 Stroke - Single acting) 2 N = (RPM ) → (For 4 Stroke - Double acting) 3. BRAKE POWER BP = PmbπLD 2 Nn' KW 4(60) where: Pmb - brake mean effective pressure in KPa N = (RPM ) → (For 2 Stroke - Single acting) N = 2(RPM) → (For 2 Stroke - Double acting) (RPM) N= → (For 4 Stroke - Single acting) 2 N = (RPM ) → (For 4 Stroke - Double acting) BP = 2 πTN KW 60,000 where: T - brake torque in N-m N = RPM 4. FRICTION POWER FP = IP − BP 5. INDICATED MEAN EFFECTIVE PRESSURE AS' Pmi = KPa L' where: A - area of indicator card, m2 S - spring scale, KPa/m L' - length of indicator card, m 6. BRAKE TORQUE T = (P − Tare )R N - m where: P - Gross load on scales, N Tare - tare weight, N R - length of brake arm, m 7. PISTON SPEED m min 8. DISPLACEMENT VOLUME πLD 2 Nn' VD = KPa 4(60) IP VD = KPa Pmi BP VD = KPa Pmb PS = 2LN Where N = (RPM ) → (For 2 Stroke - Single acting) N = 2(RPM) → (For 2 Stroke - Double acting) (RPM) N= → (For 4 Stroke - Single acting) 2 N = (RPM ) → (For 4 Stroke - Double acting) 9. SPECIFIC FUEL CONSUMPTION a. Indicated specific fuel consumption m kg mfi = f IP KW - hr b. Brake specific fuel consumption m kg mfb = f BP KW - hr c. Combined specific fuel consumption m kg mfc = f GP KW - hr where: GP - Generator output 10. HEAT RATE (HR): Heat supplied divided by the KW produced. a. Indicated heat rate Q KJ HRi = s IP KW - hr b. Brake heat rate Q KJ HRb = s BP KW - hr c. Combined heat rate Q KJ HRc = s GP KW - hr 11. GENERATOR SPEED 120f N= RPM n Where: n - number of generator poles (usually divisible by 4) 12. MECHANICAL EFFICIENCY BP ηm = x 100% IP 13. GENERATOR EFFICIENCY GP ηg = x 100% BP 14. Indicated Thermal Efficiency 3600(IP) ei = x 100% Qs 15. Brake Thermal Efficiency 3600(BP) eb = x 100% Qs 16. Combined Thermal efficiency 3600(GP) ec = x 100% Qs 17. Indicated Engine Efficiency e ηi = i x 100% e 18. Brake Engine Efficiency e ηb = b x 100% e where: e - cycle thermal efficiency 19. Volumetric Efficiency ηv = Actual volume of air entering, Displacement Volume, m3 sec m3 sec x 100% 20. Correction Factor for Nonstandard condition a. Considering temperature and pressure effect B T Ph = Ps S h Bh Ts b. Considering temperature effect alone T Ph = Ps h T s c. Considering pressure effect alone B Ph = Ps S Bh Note: From US Standard atmosphere: 83.312h Bh = Bs − mm Hg 1000 6.5h Th = Ts K 1000 where: B - barometric pressure, mm Hg T - absolute temperature, K h - at elevation h condition s - at sea level condition 21. ENGINE HEAT BALANCE: The total heat supplied to th engine was broken down into four heat items. Q2 Q1 QS engine Q3 Q4 QS = Q1 + Q2 + Q3 + Q4 Q1 - heat converted to useful work Q2 - heat lost to cooling water Q3 - heat lost to exhaust gases Q4 - heat lost due to friction, radiation and unaccounted for Q1 = 3600(BP) KJ/hr Q2 = mwCpw(two - twi) KJ/hr Q3 = Qa + Qb KJ/hr Qa = mgCpg(tg - ta) KJ/hr Qb = mf(9H2)(2442.7) KJ/hr Q4 = QS - (Q1 + Q2 + Q3) KJ/hr H2 = 0.26 - 0.15S kgH/kgfuel 141.5 S= 131.5 + API 140 S= 130 + BeI where: Qa - sensible heat of products of combustion Qb - heat required to evaporate and superheat moisture formed from the combustion of hydrogen in the fuel tg - temperature of flue gas, C ta - temperature of air, C H2 - amount of hydrogen in the fuel kg H/kg fuel TERMS AND DEFINITIONS Diesel engine is a type of internal combustion engine that uses low grade fuel oil and which burns this fuel inside the cylinder by heat of compression. It is used chiefly for heavy-duty work. Diesel engines drive huge freight trucks, large buses, tractors, and heavy road-building equipment. They are also used to power submarines and ships, and the generators of electric-power stations in small cities. Some motor cars are powered by diesel engines. Gasoline engine - is a type of internal combustion engine, which uses high grade of oil. It uses electricity and spark plugs to ignite the fuel in the engine's cylinders. Kinds of diesel engines. There are two main types of diesel engines. They differ according to the number of piston strokes required to complete a cycle of air compression, exhaust, and intake of fresh air. A stroke is an up or down movement of a piston.These engines are (1) the four-stroke cycle engine and (2) the two-stroke cycle engine. Four Stroke Cycle Engine 1. Intake 2. Compression 3. Power 4. Exhaust In a four-stroke engine, each piston moves down, up, down, and up to complete a cycle. The first down stroke draws air into the cylinder. The first upstroke compresses the air. The second down stroke is the power stroke. The second upstroke exhausts the gases produced by combustion. A four-stroke engine requires exhaust and air-intake valves. It completes one cycle in two revolutions of the crankshaft. Two Stroke Cycle Engine 1. Intake-Compression stroke 2. Power-exhaust stroke In a two-stroke engine, the exhaust and intake of fresh air occur through openings in the cylinder near the end of the down stroke, or power stroke. The one upstroke is the compression stroke. A two-stroke engine does not need valves. These engines have twice as many power strokes per cycle as four-stroke engines, and are used where high power is needed in a small engine. It completes one cycle in one revolution of the crankshaft. Governor - is a device used to govern or control the speed of an engine under varying load conditions. Purifier - a device used to purify fuel oil and lube oil. Generator - a device used to convert mechanical energy. Crank scavenging - is one that the crankcase is used as compressor. Thermocouple - is made of rods of different metal that are welded together at one end. Centrifuge - is the purification of oil for separation of water. Unloader - is a device for automatically keeping pressure constant by controlling the suction valve. Planimeter - is a measuring device that traces the area of actual P-V diagram. Tachometer - measures the speed of the engine. Engine indicator - traces the actual P-V diagram. Dynamometer - measures the torque of the engine. Supercharging - admittance into the cylinder of an air charge with density higher than that of the surrounding air. Bridge Gauge - is an instrument used to find the radial position of crankshaft motor shaft. Piston - is made of cast iron or aluminum alloy having a cylinder form. Atomizer - is used to atomize the fuel into tiny spray which completely fill the furnace in the form of hollow cone. Scavenging - is the process of cleaning the engine cylinder of exhaust gases by forcing through it a pressure of m fresh air. Flare back - is due the explosion of a maximum fuel oil vapor and air in the furnace. Single acting engine - is one in which work is done on one side of the piston. Double acting engine - is an engine in which work is done on both sides of the piston. Triple-expansion engine - is a three-cylinder engine in which there are three stages of expansion. The working pressure in power cylinder is from 50 psi to 500 psi. The working temperature in the cylinder is from 800F to 1000F. Air pressure used in air injection fuel system is from 600 psi to 1000 psi. Effect of over lubricating a diesel engine is: Carbonization of oil on valve seats and possible explosive mixture is produced. The average compression ratio of diesel engine is from 14:1 to 16:1. Three types of piston: 1. barrel type 2. trunk type 3. closed head type Three types of cam follower: 1. flat type 2. pivot type 3. roller type Methods of mechanically operated starting valve: 1. the poppet 2. the disc type Three classes of fuel pump: 1. continuous pressure 2. constant stroke c. variable stroke Type of pump used in transferring oil from the storage to the service tanks: 1. rotary pump 2. plunger pump 3. piston pump 4. centrifugal pump Valve that is found in the cylinder head of a 4-stroke cycle engine: 1. fuel valve 2. air starting valve 3. relief valve 4. test valve 5. intake valve 6. exhaust valve Four common type of governors used on a diesel engine: 1. constant speed governor 2. variable speed governor 3. speed limiting governor 4. load limiting governor Kinds of piston rings used in an internal combustion engines: 1. compression ring 2. oil ring 3. firing ring 4. oil scraper ring Reasons of smoky engine: 1. overload 2. injection not working 3. choked exhaust pipe 4. fuel or water and leaky things Methods of reversing diesel engines: 1. sliding camshaft 2. shifting roller c. rotating camshaft Arrangements of cylinders: 1. in-line 2. radial 3. opposed cylinder 4. V 5. opposed piston Position of cylinders: 1. vertical 2. horizontal 3. inclined Methods of starting: 1. manual, crank, rope, and kick 2. electric (battery) 3. compressed air 4. using another engine Applications: 1. automotive 2. marine 3. industrial 4. stationary power 5. locomotive 6. aircraft Types of internal combustion engine: 1. Gasoline engine 2. Diesel engine 3. Kerosene engine 4. Gas engine 5. Oil-diesel engine Methods of ignition: 1. Spark 2. Heat of compression Reasons for supercharging: 1. to reduce the weight to power ratio 2. to compensate the power loss due to high altitude Types of superchargers: 1. engine-driven compressor 2. exhaust-driven compressor 3. separately-driven compressor Auxiliary systems of a diesel engine: 1. Fuel system a. fuel storage tank b. fuel filter c. transfer pump d. day tank e. fuel pump 2. Cooling system a. cooling water pump b. heat exchanger c. surge tank d. cooling tower e. raw water pump 3. Lubricating system: a. lub oil tank b. lub oil pump c. oil filter d. oil cooler e. lubricators 4. Intake and exhaust system a. air filter b. intake pipe c. exhaust pipe d. silencer 5. Starting system a. air compressor b. air storage tank Advantages of diesel engine over other internal combustion engines: 1. low fuel cost 2. high efficiency 3. needs no large water supply 4. no long warm-up period 5. simple plant layout Types of scavenging: 1. direct scavenging 2. loop scavenging 3. uniflow scavenging Color of the smoke: 1. efficient combustion - light brown baze 2. insufficient air - black smoke 3. excess air - white smoke Causes of black smoke: 1. fuel valve open too long 2. too low compression pressure 3. carbon in exhaust pipe 4. overload on engine Causes of white smoke: 1. one or more cylinders not getting enough fuel 2. too low compression pressure 3. water inside the cylinder ENGINE FOUNDATION Functions of a Foundation: Support the weight of the engine. Maintain proper alignment with the machinery and Absorb the vibration produced by unbalanced forces created by reciprocating revolving masses. Materials: Mixture: 1 : 2 : 4 1 part Cement 2 parts sand 4 parts broken stone or Gravel For good firm soil, reinforced concrete foundations for large engines may use a leaner mixture down to 1:3:6 Soil Bearing Pressure: The safe loads vary from about 4,890 kg/m 2 for alluvial soil or wet clay, to 19,560 kg/m2 for gravel, coarse sand and dry clay. (12,225 kg/m2 is assumed to be safe load average). In computation 2,406 kg/m2 may be used as weight of concrete. Depth: The foundation depth maybe taken as a good practical rule, to be 3.2 to 4.2 times the engine stroke; the lower factor for wellbalanced multi-cylinder engines and increased factor for engines with fewer cylinders or on less firm soil. Weight: The minimum weight required to absorb vibration could be expressed as a function of the reciprocating masses and the speed of the engine. However, for practical purposes it is simpler to use the empirical formula. Volume: If the weight and speed of the engine is not known, the volume of concrete for the foundation may be estimated from the data in the table. Anchor Bolts: To prevent pulling out of the bolts when the nuts are tightened, the length embedded in concrete should be equal to at least thirty (30) times the bolt diameter. The upper ends are surrounded by a 50 mm or 75 mm sheet metal pipe, 460 mm to 610 mm long to permit them to be bent slightly to fit the holes of the bedplate. FORMULA: WF = e (WE) N Where: WF – weight of foundation in kgs WE – weight of engine in kgs e – empirical coefficient N – engine speed in RPM Values of e Type of Engine Single Acting Single Acting Single Acting Single Acting Single Acting Single Acting Single Acting Double acting Double acting Cylinder Arrangement Vertical Vertical Vertical Vertical Horizontal Horizontal Duplex Horizontal Twin Duplex Horizontal Horizontal Twin Tandem No. of Cylinders 1 2 3 4, 6, 8 1 2 4 1, 2 4 e 0.15 0.14 0.12 0.11 0.25 0.24 0.23 0.32 0.20 Volume of Concrete Foundation (Cubic Feet per HP) No. of Cylinders 1 2 3 High speed engine 4.0 2.5 2.0 Medium speed engine 5.0 3.1 2.5 Low speed engine 6.0 4.0 3.0 Note: 1 cubic meter (m3) = 35.315 ft3 1 Horsepower = 0.746 KW 4 1.7 2.1 2.6 5-8 1.5 1.9 2.3 General Requirements 1. All heavy machinery shall be supported on solid foundation of sufficient mass and base area to prevent or minimize the transmission of objectionable vibration to the building and occupied space and to maintain the supported machine at its proper elevation and alignment. 2. Foundation mass should be from 3 to 5 times the weight of the machinery it is supposed to support. If the unbalanced inertial forces produced by the machine can be calculated, a mass of weight equal to 10 to 20 times the forces should be used to dampen vibration. For stability, the total combined engine, driven equipment and foundation center of gravity must be kept below the foundation’s top. 3. the weight of the machine plus the weight of the foundation should be distributed over a sufficient soil area which is large enough to cause a bearing stress within the safe bearing capacity of the soil with a factor of safety of 5. 4. Foundation should be isolated from floor slabs and building footings by at least 25 mm around its perimeter to eliminate transmission of vibration. Fill opening with water tight-mastic. When installing machinery above grade level of a building, additional stiffness must be provided on its structural members of the building to dampen machine vibration. 5. Foundations are preferably built of concrete in the proportions of one (1) measure of Portland Cement to two (2) measures of sand and four (4) measures of screened crushed stones. The machine should not be placed on thefoundation until ten (10) days have elapsed or operated until another ten (10) days have passed. 6. Concrete foundation should have steel bar reinforcements placed both vertically and horizontally, to avoid thermal cracking. Weight of reinforcing steel should be from ½ % to 1 % of the weight of the foundation. 7. Foundation bolts of specified size should be used and surrounded by a pipe sleeve with an inside diameter of at least three (3) times the diameter of the anchor bolt and a length of at least eighteen (18) times the diameter of the bolt. No foundation bolts shall be less than 12 mm diameter. 8. Machine should be leveled by driving wedges between the machine’s base and concrete foundation and with The aid of a spirit level. Grout all spaces under the machine bed with a thin mixture of one (1) part cement and one part sand. The level wedges should be removed after grout has thoroughly set and fill wedges holes with grout. SAMPLE PROBLEMS 1. A 2 - stroke, 4 - cylinders, 38 cm x 53 cm diesel engine is guaranteed to deliver 522 KW at 300 rpm. The fuel rate is 0.26 kg/KW-hr. If the heating value of the fuel is 44,320 KJ/kg Calculate: a) the brake thermal efficiency (32%) b) the brake mean effective pressure (422 KPa) c) suction displacement in m3/min-KW of shaft power (0.15) d) heat supplied to cylinder per Liter of displacement Given: 2-stroke, n’ = 4; D = 0.38 m; L = 0.53 m; BP = 522 KW; N = 300 RPM mFB = 0.26 kg/KW-hr; HV = 44,320 KJ/kg 3600BP 3600BP 3600 a. eb = = = = 31.2% . Qs mF (HV) mFB (HV) PmBπLD 2 Nn' KW 4(60) N = RPM (for 2 - stroke, single acting) 240(BP) PmB = = 434 KPa πLD 2 Nn' b. BP = . c. BP = PmB(VD ) VD 1(60) m3 = = 0.14 BP PmB min - KW d. 2. QS m (HV) KJ mFB (BP)(HV)PmB mFB (HV)PmB = F = = KJ/L = 1.4 KJ/L VD BP(3600) m3 BP(3600) (3600)(1000) PmB Find the volume in Liters needed for a two weeks supply of 26API fuel oil to operate a 750 KW engine 70 % of the time at full load, 10 % at 3/4 load and idle 20% of the time. Fuel rate is 0.25 kg/KW-hr at full load and 0.24 kg/KW-hr at 3/4 load. Temperature of oil is 21C. T = 2weeks(7 days)(24 hours) = 336 hrs m F = 336(0.70)0.25(750) + 0.10(336)(0.75)(750)(0.24) = 48,636 kg 141.5 = 0.898 131.5 + 26 S @ t = 0.898 − 0.0007(21 − 15.56) = 0.895 kg kg ρ = 895 3 = 0.895 L m 48,636 VF = = 54,342 Liters 0.895 For Fuel Tank Design H = 1.25D D = 0.75H S= Sample Problem (ICE & ENGINE HEAT BALANCE) A single cylinder, single acting, 30.5 cm by 46 cm, 4-stroke cycle diesel engine for a 3 storey office building was tested for one (1) hour and the following data were obtained: • Fuel consumed 7.5 kg • Total revolutions 12,120 • Jacket Water 674 kg • Rise in temperature of Cooling water 28C • Area of Indicator Card 5.56 cm2 • Length of Indicator Card 7 cm • Spring Scale 815 KPa/cm • Torque 1,139 N-m • Heating Value of fuel 44,200 KJ/kg Find: a. The IP, BP, and Mechanical efficiency b. The indicated and brake specific fuel consumption c. The %age of total heat supplied converted into brake power d. The %age of total heat absorbed by jacket water e. The %age of heat lost to friction, exhaust gases, radiation and etc. Solution: a. 2πTN 2π(1139)12,120 BP = = = 24 KW 60,000 60,000(60) A' S 5.56(815) Pmi = = = 647.34 KPa L' 7 Pmi πLD 2 Nn' 4(60) 12120 N= = 202 RPM 60 647.34π(0.46)(0.305) 2 (202)1 IP = = 37 KW 4(60)2 BP 24 ηm = x 100% = = 65% IP 37 IP = b. m F 7.5 kg = = 0.203 IP 37 KW - hr m 7.5 kg = F = = 0.3125 BP 24 KW - hr m Fi = m FB c. d. e. Qs = mF(HV) = 7.5(44,200) = 331,500 KJ/hr Q1 = %age of heat converted to work 24(3600) Q1 = x100% = 26 % 331,500 Qw = heat absorbed by cooling water Qw = mw(CPW) (tWB – tWA) Qw = 674(4.187)(28) = 79,017.064 KJ/hr Q2 = %age of total heat absorb by cooling or jacket water 79,017.064 Q2 = x 100% = 24 % 331,500 Q3 = %age of total heat lost to exhaust gas, friction, radiation and etc. Q3 = 100 –(Q1 + Q2) = 100 – (26 + 24) = 50 % Sample Problem (ICE & ENGINE HEAT BALANCE) A diesel generator set with a generator capacity of 1500 KW has a combined specific fuel consumption of 0.28 kg/KW-hr. The engine uses fuel oil at 28API with an air-fuel ratio of 15:1. Atmospheric air in the plant averages 35C and 1 atmosphere pressure. Exhaust gas temperature is 450C and generator efficiency is 92%. Cooling water is available at 16C and leaves the engine at 32C. If the heat loss due to incomplete combustion, friction , radiation and unaccounted for amounts to 9% of the heat supplied by fuel, determine the four heat items in KJ/hr and the cooling water required by the engine in L/sec. (C pg = 1.026 KJ/kgC) 141.5 141.5 = = 0.887 131.5 + ο API 131.5 + 28 H 2 = 0.26 − 0.15S = 0.26 − (0.15)(0.887) = 0.127 kgH 2 / kgf uel S= LHV = HHV − Q L Q L = 2442.7(9H 2 ) = 2442.7(9)(0.127) = 2,790.42KJ / kg HHV = 51,716 − 8793.8(S) 2 HHV = 51,716 − 8793.8(0.887) 2 = 44,797KJ / kg LHV = HHV - Q L KJ/kg LHV = 44797 - 2790.42 = 42,006.58KJ / kg Q1 = 3600(BP) KJ/hr Q2 = mwCpw(two - twi) KJ/hr Q3 = Qa + Qb KJ/hr Qa = mgCpg(tg - ta) KJ/hr Qb = mf(9H2)(2442.7) KJ/hr Q4 = QS - (Q1 + Q2 + Q3) KJ/hr 150 KJ (3600) = 5,869,565.2 0.92 hr Q3 = Qa + Qb Q1 = Q a = m g C pg ( t g − t a ) mg = ma + m F ma = 15 mF kg hr kg m a = 15(420) = 6300 hr kg m g = 6,720 hr m F = 0.28(1500) = 420 KJ hr KJ Q b = 420(9)(0.127)(2442.7) = 1,171,976.4 hr KJ Q3 = 4,0333,285.2 hr KJ Qs = 420(42,006.58) = 17,642,763.6 hr KJ Q 4 = 0.09(17,642,763.6) = 1,587,848.724 hr Q a = 6720(1.026)(450 − 35) = 2,861,308.8 Qs = Q1 + Q 2 + Q3 + Q 4 Q 2 = Qs − (Q1 + Q3 + Q 4 ) = 6,152,064.476 KJ hr Q 2 = m w (4.187)(32 − 16) m w = 91,833 kg hr at 16C : ρw = 999 kg m3 91,833 hr 1000L L mw = of cooling water = 26 3 999 3600 m sec COMBUSTION ENGINEERING QUIZ NO. 1(April 15, 2019) Name _______________________ Problem No. 1 A fuel represented by C7H16 is oxidized with 20% excess air and the mass of fuel required for combustion is 50 kg/hr. Determine the mass flow rate of the products in kg/hr. Fuel : C 7 H16 e : 20% kg hr Combustion with 100% TA C 7 H16 + aO 2 + a(3.76)N2 → bCO2 + cH 2 O + a(3.76)N2 m Fuel : 50 a = n + 0.25m = 11 b=n=7 c = 0.5m = 8 Combustion with EA (e = 0.20) C 7 H16 + (1.20)aO 2 + (1.20)a(3.76)N2 → bCO2 + cH 2 O + dO 2 + (1.20)a(3.76)N2 d = e(n + 0.25m) = 2.2 Combustion Equation C 7 H16 + 13O 2 + 49.632N 2 → 7CO2 + 8H 2 O + 2.2O 2 + 49.632N 2 Mass of Products (m products) m products = 7(44) + 8(18) + 2.2(32) + 49.632(28) = 1,912.10 kg Mass of Products per kg of fuel m products 1,912.10 1,912.10 kg Products = = = 19.12 m Fuel 12(7) + 16 100 kgFuel M Pr oducts − mass flow rate of products M Products = 19.12(50) = 956 kg hr Problem No. 2 The analysis of the natural gas showed the following percentages by volume: C2H6 = 9%; CH4 = 90%; CO2 = 0.2 % and N2 = 0.8 %. Find the volume of air required per cu,m. of gas if the gas and air are at temperature of 16C and a pressure of 101.6 KPa. Combustion with 100% TA (Basis :100 moles of fuel) 9C 2 H 6 + 90CH4 + 0.2CO2 + 0.8N 2 + aO 2 + a (3.76) N 2 → bCO2 + cH 2 O + dN 2 Carbon Balance 2(9) + 90 + 0.2 = b b = 108.2 Hydrogen Balance 6(9) + 4(90) = 2c c = 207 Oxygen Balance 0.2(2) + 2a) = 2b + c a = 211.5 Nitrogen Balance 2(0.8) + a(3.76)2 = 2d d = 796.04 9C 2 H 6 + 90CH4 + 0.2CO2 + 0.8N 2 + 211.5O 2 + 795.24 N 2 → 108.2CO2 + 207H 2 O + 796.04 N 2 n Air = 211.5+ = 795.24 = 1,006.74 Moles n Gas = 100 PV = n RT n RT P At the same temperaru te and pressure, the mole ratio is equal to volumetri c ratio V= m 3 of Air 1,006.74 = = 10.06 3 100 m of fuel Problem No. 3 A fuel with a molal analysis of 80% C12H26 and 20% C14H30 is burned with 30% excess air. The flue gas is at P = 101 KPa. Dtermine a. the combustion equation b. the actual air-fuel ratio c. the partial of H2O and DPT in the products Combustion with 100% TA (basis; 100 moles of fuel) 80C12H 26 + 20 C14H 30 + aO 2 + a(3.76)N 2 → bCO2 + cH 2 O + a(3.76)N 2 80(12) + 20(14) = b b = 1240 80(26) + 20(30) = 2c c = 1340 2a = 2b + c a = 1910 Combustion with EA (e = 0.30) 80C12H 26 + 20 C14H 30 + (1.30)aO 2 + (1.30)a(3.76)N2 → bCO2 + cH 2 O + dO 2 + (1.30)a(3.76)N2 1.30a (2) = b(2) + c + 2d d = 573 Combustion Equation 80C12H 26 + 20 C14H 30 + 2483O 2 + 9336.08N 2 → 1240CO2 + 1340H 2 O + 573O 2 + 9336.08N 2 2483(32) + 9336.08(28) A = 19.41 Actual = 80(170) + 20(198) F n Pr oducts = 1240 + 1340 + 573 + 9336.08 = 12,489.08 PH2O 1340 = P 12,489.08 PH2O 1340 = 101 12,489.08 PH2O = 10.84 KPa DPT = tsat at 10.84 KPa DPT = 47.417C COMBUSTION ENGINEERING QUIZ NO. 2 (April 23, 2019) Name ______________________________ Problem No. 1 The mass analysis of hydrocarbon fuel A is 88.5% Carbon and 11.5% Hydrogen. Another hydrocarbon fuel B requires 6% more air than fuel A for complete combustion. Calculate the mass analysis of Fuel B. For Fuel A A = 11.44(0.885) + 34.32(0.115) = 14.07 F For Fuel B A = (1.06)(14.07) = 14.915 F C + H =1 C = (1 − H) A = 11.44(1 − H) + 34.32H = 14.915 F 14.915 − 11.44 = (34.32 − 11.44)H H = 0.1519 = 15.19% C = (1 − .1519) = 0.8481 = 84.81% Problem No. 2 A diesel engine uses a hydrocarbon fuel represented by C12H26 and is burned with 30% excess air. The air and fuel is supplied at 1 atm and 25C. Determine f. the actual air-fuel Ratio g. the m3 of CO2 formed per kg of fuel if the product temp. is 400C and a pressure of 1 atm. h. The M and R of the Products i. The M and R of the dry flue gas j. If 1.5 moles of carbon oxidizes to CO, determine the molecular weight of the resulting products Combustion with 130%TA C12H 26 + (1.30)aO 2 + (1.30)a(3.76)N 2 → bCO2 + cH 2 O + dO 2 + (1.30)a(3.76)N 2 b=n b = 12 a = n + 0.25m = 18.5 c = 0.5m = 13 d = e(n + 0.25m) = 5.55 C12H 26 + 24.05O 2 + 90.428N 2 → 12CO2 + 13H 2 O + 5.55O 2 + 90.428N 2 (1.30)137.28(n + 0.25m) A = = 19.42 12m + m F Actual 12(8.3143)(400 + 273) VCO 2 = = 662.7 m 3 101.325 VCO 2 662.7 = = 3.9 m Fuel 12(12) + 26 n Pr oducts = 12 + 13 + 5.55 + 90.428 = 120.98 M= m Pr oducts 12(44) + 13(18) + 5.55(32) + 90.428(28) kg = = 28.7 n Pr oducts 120.98 kg mol R= 8.3143 KJ = 0.29 28.7 kg - K m Dry flue gas = 12(44) + 5.55(32) + 90.428(28) = 104.09 M Dry Flue Gas = 12 + 5.55 + 90.428 kg = 29.82 104.09 kg mol Combustion with CO and with 100%TA C12 H 26 + aO 2 + a(3.76)N 2 → bCO2 + cH 2 O + 1.5CO + a(3.76)N 2 12 = b + 1.5 b = 12 - 1.5 = 10.5 26 = 2c c = 13 2a = 2b + c + 1.5 c 1.5 a = b+ + = 17.75 2 2 Combustion with CO and with EA (e = 0.30) C12 H 26 + (1.30)aO 2 + (1.30)a(3.76)N 2 → bCO2 + cH 2 O + 1.5CO + dO 2 + (1.30)a(3.76)N 2 By oxygen balance d = 5.325 C12 H 26 + 23.075O 2 + 86.762N 2 → 10.5CO 2 + 13H 2 O + 1.5CO + 5.325O 2 + 86.762N 2 n Pr oducts = 10.5 + 13 + 1.5 + 5.325 + 86.762 = 117.09 M= 10.5(44) + 13(18) + 1.5(28) + 5.325(32) + 86.762(28) kg = 28.51 117.09 kg mol COMBUSTION ENGINEERING QUIZ NO. 3 (April 24, 2019) Name ___________________________________ Problem 1: Calculate the theoretical oxygen and air required to burn 1 kgmol of carbon, and 1 kgmol of Hydrogen. H 2 + 1 O 2 → H 2O 2 C + O 2 → CO 2 2 + 16 → 18 12 + 32 → 44 3 + 8 → 11 kgO 2 8 = = 2.67 kgC 3 kgAir = 11.44 kgC 1+ 8 → 9 kgO 2 8 = =8 KgH 1 kgAir = 34.32 KgH Problem 2: Calculate the theoretical Oxygen--fuel ratio and Air--fuel ratio on a mass basis for the combustion of ethanol, C2H5OH. Combustion with 100% TA C 2 H 5OH + aO 2 + a (3.76) N 2 → bCO2 + cH 2 O + a (3.76) N 2 2=b 5 + 1 = 2c c=3 1 + 2a = 2b + c 2(2) + 3 − 1 a= =3 2 C 2 H 5OH + 3O 2 + 11.28N 2 → 2CO2 + 3H 2 O + 11.28N 2 kgOxygen 3(32) 96 = = = 2.09 kgFuel 124 + 5 + 16 + 1 46 kgAir 3(32) + 11.28(28) = = 8.95 kgFuel 124 + 5 + 16 + 1 Problem 3: Determine the molal analysis of the products of combustion when octane C 8H18 is burned with 100% excess air. Combustion with EA (e = 100%) C8 H18 + (1 + 1)aO 2 + (1 + 1)a (3.76) N 2 → bCO2 + cH 2 O + dO 2 + (1 + 1)a (3.76) N 2 a = n + 0.25m b=n c = 0,5m d = e(n + 0.25m) C8 H18 + 24.5O 2 + 92.12 N 2 → bCO2 + cH 2 O + dO 2 + (1 + 1)a (3.76) N 2 C8 H18 + 25O 2 + 94 N 2 → 8CO2 + 9H 2 O + 12.5O 2 + 94 N 2 n Pr oducts = 8 + 9 + 12.5 + 94 = 123.5 8 y CO 2 = x100% = 6.48% 123.5 9 y H 2O = x100% = 7.29% 123.5 12.5 y O2 = x100% = 10.12% 123.5 94 y N2 = x100% = 76.11% 123.5 Problem 4: A certain fuel has the composition C10H22. If this fuel is burned with 50% excess air, what is the composition of the products of combustion? Combustion with EA (e = 50%) C10H 22 + 23.25O 2 + 87.42 N 2 → 10CO2 + 11H 2 O + 7.75O 2 + 87.42N 2 a = n + 0.25m b=n c = 0,5m d = e(n + 0.25m) Problem 5: A sample of pine bark has the following ultimate analysis, percent by mass: C = 53.4% ; H2 = 5.6% ; O2 = 37.9% ; N2 = 0.1% ; S = 0.1% ; Ash = 2.9%. This bark will be used as a fuel by burning it 30% excess air. Determine the actual airfuel ratio. Fuel C H2 O2 N2 S H20 Ash Total UA 53.4 5.6 37.9 0.1 0.1 0 2.9 100 Ashless 55 5.8 39 0.103 0.103 0 0 100 O A = 11.44C + 34.32 H 2 − 2 + 4.29S = 6.6 8 F T heoretical A A = (1 + e) = 8.58 F Actual F T heoretical COMBUSTION ENGINEERING Activity No. 4 (APRIL 29, 2019) NAME __________________________________ Problem No. 1 A combustor receives 340 m3/min of natural gas having a volumetric chemical composition of 15% C 2H6 and 85% CH4 that requires 25% excess air. Air and fuel enters the combustor at 25C (298 K)and 101 KPa and products of combustion leaves at 1100 K. Emission test gives that 2 moles of CO and 1 mole NO is found in the products. Determine f. The actual combustion equation g. The actual air – fuel ratio h. The heating value of the fuel (HP – HR) KJ/kg i. The mass flow rate of fuel in kg/min j. The volume flow rate of emission gases (CO2, CO and NO) in m3/hr C2H6: M = 30; Cp = 1.7549 KJ/kg-K; Cv = 1.4782 KJ/kg-K CH4: M = 16; Cp = 2.1377 KJ/kg-K; Cv = 1.6187 KJ/kg-K Combustion with 100% TA Basis :100 moles of fuel 15C 2 H 6 + 85CH4 + aO 2 + a(3.76)N 2 → bCO2 + cH 2 O + 2CO + 1NO + dN 2 15C 2 H 6 + 85CH4 + 222O 2 + 834.72N 2 → 113CO2 + 215H 2 O + 2CO + 1NO + 834.22 N 2 Combustion with EXCESS AIR(e = 0.25) Basis :100 moles of fuel 15C 2 H 6 + 85CH4 + (1.25)222O 2 + (1.25)834.72N 2 → 113CO2 + 215H 2 O + 2CO + 1NO + fO 2 + gN 2 15C 2 H 6 + 85CH4 + 227.5O 2 + 1,043.4 N 2 → 113CO2 + 215H 2 O + 2CO + 1NO + 55.5O 2 + 1,042.9 N 2 227.5(32) + 1,043.4(28) A = = 21.05 15(30) + 85(16) F Actual Problem No. 2 Calculate the theoretical air – fuel ratio of the Hydrocarbon Fuel in the table below. Fuel C8H18 C7H16 C4H10 C9H20 C11H24 Theoretical (By Mass) 15.05 15.10 15.38 15.02 14.96 A/F Ratio COMBUSTION ENGINEERING Activity No. 4 (APRIL 30, 2019) Special Quiz Name ___________________________________ A European made diesel engine uses liquid Octadecane (C18H38) fuel for power generation. This fuel is burned with 30% excess air requirement. Air and fuel enters the engine at 25C (298 K) and 101 KPa and products of combustion leaves at 1200 K. It is found that the products contains 2 moles of CO and 2 moles of NO during the test. Determine a. The actual combustion equation b. The actual air – fuel ratio c. The heating value of the fuel (HP – HR) KJ/kg if (hf)C18H38 = -505,400 KJ/kgmol d. The volume flow rate of emission gases (CO2, CO and NO) in m3/hr if the fuel consumption is 250 kg/hr Combustion with 100% TA Basis :1 mole of fuel C18 H 38 + aO 2 + a(3.76)N 2 → bCO 2 + cH 2 O + 2CO + 2NO + dN 2 By Balancing equation C18 H 38 + 27.5O 2 + 103.4 N 2 → 16CO 2 + 19H 2 O + 2CO + 2NO + 102.4 N 2 Combustion with 30% EA C18 H 38 + 37.75O 2 + 134.42 N 2 → 16CO 2 + 19H 2 O + 2CO + 2NO + 8.25O 2 + 133.42 N 2 37.75(32) + 134.42(28) A = = 19.32 12(18) + 38 F Actual n EG = 16 + 2 + 2 = 20 20(8.3143)(1200) = 1,975.68 m 3 → Volume of emission gases 101 V EG 1,975.68 = = 7.78 kg of Fuel 254 VEG = VFEG = 7.78(250) = 0.031 m3 of Emission Gases hr COMBUSTION ENGINEERING Activity No. 5 (May 02, 2019) NAME __________________________________ A hydrocarbon Fuel C7H16 (n-Heptane) was tested in a laboratory in order to determine its LHV and HHV. The fuel is burned with 50% excess air requirement for complete combustion. Air and fuel enters the apparatus at 25C and 101 KPa, while the products of combustion leaves the apparatus at 600 K. Determine a. the combustion equation b. the LHV in KJ/kg of fuel c. the HHV in KJ/kg of fuel hf of C7H16 = -187,900 KJ/kgm For HHV For LHV COMBUSTION ENGINEERING Activity No. 6 (May 03, 2019) NAME __________________________________ Multiple Choice Instruction: Write the letter, which corresponds to the correct answer in the table below. 1. A hydrocarbon fuel represented by C8H18 is burned with air. Its gas constant in KJ/kg-K is equal to; a. 0.073 b. 0.286 c. 0.0826 d. 0.187 2. A gaseous mixture has the following volumetric analysis O2, 30%; CO2, 40% N2, 30%. Determine its molecular weight in kg/kgmol. a. 25.6 b. 35.6 c. 28.9 d. 30.2 3. The products of combustion of an automotive engine using a diesel fuel has an Orsat analysis as follows; CO 2 = 12.5%; O2 = 3.5%; CO = 0.5%; N2 = 83.5%. The gas constant of the dry flue gas is equal to; a. 0.287 b. 1.0045 c. 0.1889 d. 1.007 4. A newly designed high speed European car uses high grade gasoline fuel represented by C 8H18. If this fuel is burned with 30% excess air, determine the actual air-fuel ratio. a. 20.5 b. 10.87 c. 15.8 d. 19.6 5. A fuel represented by C7H16 is oxidized with 20% excess air and the mass of fuel required for combustion is 50 kg/hr. Determine the mass flow rate of the products in kg/hr. a. 956.05 b. 906.05 c. 806.07 d. 856.07 6. There are 20 kg of flue gas formed per kg of fuel burned for the combustion of C 12H26. What is the percent excess air. a. 27.17 b. 16.56 c. 26.67 d. 8.21 7. For a certain ideal gas mixture, R = 0.270 KJ/kg-k and k = 1.3. Determine the mass of the mixture in kg for 10 moles of the mixture. a. 408 b. 308 c. 508 d. 208 8. Determine the molecular weight of a products if Cp = 1.1 KJ/kg-K and k = 1.3. a. 28.75 b. 26.75 c. 32.75 d.39.75 9. Determine the mass ratio C/H of a hydrocarbon fuel with a chemical formua of C 16H32. a. 8 b. 10 c. 4 d. 6 10. The Dalton’s Law of partial pressure is called the: a. Law of additive volume b. Law of additive mass c. Law of additive moles d. Law of additive pressure Problem: A Fuel Oil belonging to the paraffin family that is 85%C and 15%H is burned in an internal combustion engine and requires 20% excess for complete combustion. Determine; 11) The fuel chemical formula a. C17H36 b. C12H26 c. C10H22 d. C14H30 12) The actual air-fuel ratio a. 14.25 b. 17.85 c. 19.26 d. 20.26 13) The kg of CO2 formed per kg of fuel a. 2.118 b. 1.117 c. 3.117 d. 4.118 14) The partial pressure of H2O if the total pressure of the products is 101 KPa a. 18.72 b. 10.93 c. 75.23 d. 11.54 15) The gas constant R of the products in KJ/kg-K a. 0.2895 b. 0.3762 c. 0.2004 d. 0.3008 ANSWER TABLE 1 a 2 b 3 a 4 d 5 a 6 7 8 9 10 a b c d d 11 12 13 14 15 a b c d a COMBUSTION ENGINEERING MIDTERM EXAM Name ______________________________ Problem A medium size internal combustion engine power plant is situated at an altitude of 800 m above sea level. The engine is 4 – stroke diesel engine using C16H34 with 50% excess air required for combustion. The plant produces 1.5 MW of electrical energy with a specific fuel consumption of 0.30 kg/KW – hr. Sea level condition is P = 760 mm Hg and T = 293 K. Design the required Height and diameter of the smoke stack in the plant with an actual draft of 25 mm of H 2O and assume 10% losses and average flue gas temperature of 350C . Diameter Generator Output = 1,500 KW Height Fuel and air Diesel Engine At 800 m above sea level P = 92.21 KPa T = 287.8 K P kg ρ air = = 1.12 3 RT m Combustion of C16H 34 with 50% excess air C16H 34 + 36.75O 2 + 138.18N 2 → 16CO2 + 17H 2 O + 12.25O 2 + 138.18N 2 16(44) + 17(18) + 12.25(32) + 138.18(28) kg = 28.74 16 + 17 + 12.25 + 138.18 kgm 8.3143 KJ R Pr oducts = = 0.289 M kg - K 183.43(8.3143)(350 + 273) VPr oducts = = 10,304.005 m 3 92.21 3 10,304.005 (0.30)(1500) hr = 5.7 m Q Pr oducts = 12(16) + 34 3600 sec sec M Pr oducts = 92.21 kg = 0.51 3 (0.289)(350 + 273) m D a = D t − 0.10D t = 25 mm water ρ Pr oducts = D t = 28.09 mm 28.09(1000) = 54.85 m of flue gas 1000(0.51) m v = 2gh g = 32.80 sec 1000H ρ air - ρ gas Dt = mm water ρ water hg = ( H = 46.05 m ) Qg = π 2 D (kv) 4 D= 4(5.7) = 0.7 m π(0.40)(32.80) SPECIAL EXAM MIDTERM Name _______________________________ A coal fired steam power plant consumes Ten Metric Tons of coal per day. The coal has an as – received Ultimate Analysis of C = 75% ; H2 = 5 % ; O2 = 7.0 %; N2 = 1.5 %; S = 2.0 %; M = 2.5 % and Ash = 7 %. This coal is burned with 50% excess air in CFB boiler. Determine a. The Ultimate Analysis on an ash-less basis b. The molal analysis on an ash-less basis c. The combustion equation d. The actual air-fuel ratio e. The required height and diameter of the smoke stacks if, Da = 30 mm H2O; Dlosses = 12%; k = 0.40 Air and fuel temp. = 298 K; Flue gas temp. = 400C; P = 101 KPa Fuel U.A. C H2 O2 N2 S H2O Ash 75.00 5.00 7.00 1.50 2.00 2.50 7.00 100 U.A. (Ashless) 80.65 5.38 7.53 1.61 2.15 2.69 100 Mi Xi/Mi 12 2 32 28 32 18 - 0.07 0.03 0.002 0.0006 0.0007 0.0015 - Molal Analysis 67.76 27.10 2.37 0.58 0.68 1.51 100 Combust ion equation w ith 50% EA 67.76C + 27.10H2 + 2.37O2 + 0.58N2 + 0.68S + 1.51H2O → Fuel 119.43O2 + 449.05N 2 → Air 67.76CO2 + 28.61H 2O + 0.68SO2 + 39.81O 2 + 449.63N 2 → Pr oducts 0.0753 A = (1.50) 11.44(0.8065) + 34.32 0.0538 − + 4.29(0.0215) 8 F Actual A = 16.26 F Actual 101 kg ρ air = = 1.18 3 0.287(298) m kg ρ water = 1000 3 m 67.76(44) + 28.61(18) + 0.68(64) + 39.81(32) + 449.63(28) M Pr oducts = = 29.67 67.76 + 28.61 + 0.68 + 39.81 + 449.63 KJ R Pr oducts = 0.280 kg - K 101 kg ρ Gas = = 0.54 3 0.280(400 + 273) m D a = D t − 0.12D t Da 30 = = 34.09 mm 1 − Losses 1 − 0.12 34.09(1000) h gas = = 63.65 m of gas 1000(0.54) m v = 2g(hg) = 35.34 sec m v' = kv = 0.40(35.34) = 14.14 sec 10Mton 1000kg day hr kg m Fuel = = 0.116 day Mton 24hrs 3600 sec sec kg m Air = 16.26(0.116) = 1.189 sec kg m FlueGas = m Air + m Fuel = 2.002 sec 2.002 m3 Q FlueGas = = 3.74 0.54 sec 1000H(ρ Air − ρ Gas ) Dt = mm WG ρ Water Dt = H = 52.83 m π Q FlueGas = D 2 ( v' ) 4 D = 0.58 Meters COMBUSTION ENGINEERING FINAL EXAM SERIES S1 Name ___________________________________ Problem No. 1 In an air standard Otto cycle, the compression ratio is 7 and the compression begins at 35C and 100 KPa. The maximum temperature of the cycle is 1100C. Find (a) the temperature and the pressure at various points in the cycle, (b) the heat supplied per kg of air, (c) work done per kg of air, (d) the cycle efficiency and (e) the MEP of the cycle. Q A = mC v (T3 − T2 ) Cv = R KJ = 0.7175 k −1 kg − K KJ kg KJ Q R = mC v (T4 − T1 ) = 231.32 kg KJ W = Q A − Q R = 271.78 kg W e= x100% = 50.08% QA Q A = mC v (T3 − T2 ) = 503.82 r=7 P1 = 100KPa T1 = 35 + 273 = 308K T3 = 1100 + 273 = 1,373K T2 = T1 (r ) k −1 = 670.8K P2 = P1 (r ) k = 1,524.5KPa P2 P3 = T2 T3 1 e = 1 − k −1 x100% = 50.08% (r ) P3 = 3,120.4KPa Pm = 1 T4 = T3 k −1 = 630.42K (r ) k 1 P4 = P3 = 204.67KPa r W VD RT1 1 m3 VD = 1 − = 0.758 P1 r kg Pm = 358.6 KPa Problem No. 2 In a Diesel cycle, the compression ratio is 15. Compression begins at 100 KPa, 40C. The heat added is 1,675 KJ/kg. Find (a) the maximum temperature in the cycle, (b) work done per kg of air (c) the cycle efficiency (d) the temperature at the end of the isentropic expansion (e) the cut-off ratio and (f) the MEP of the cycle. r = 15 P1 = 100 KPa T1 = 40 + 273 = 313 K KJ QA = 1,675 kg T 2 = T1(r )k −1 = COMBUSTION ENGINEERING FINAL EXAM SERIES S2 Name ___________________________________ Problem No. 1 A 40 KW blast furnace engine shows by test a gas consumption of 4.2 m 3/KW-hr. Heating value of gas is 3,350 KJ/m 3. Mechanical efficiency of the gas engine is 86%, Calculate: a) The brake thermal efficiency b) Indicated thermal efficiency c) Heat rate in KJ/KW-hr d) If the heat rejected to cooling water is 28% of the heat generated in engine cylinder, determine the quantity of cooling water in L/hr to be circulated if the allowable rise in temperature of the cooling water is 10C Problem No. 2 A mechanical draft cooling tower of a Diesel Power Plant is required to cool 15 kg/sec of water at 65C entering temperature to a temperature of 35C. Atmospheric air at P = 97 KPa; tdA =28C and twA = 22C enters the cooling tower and leaves at tdB = 60C (Psat = 19.925 KPa) and RH = 90%. If make-up water is supplied at 35C (hf = 146.51 KJ/kg) , Calculate a) The kg/sec of dry air in the tower b) c) d) e) f) h) The make-up water flow rate in kg/hr The m3/sec capacity of Force draft fan at the bottom of the tower The actual cooling Range (ACR) the cooling tower approach (CTA) the theoretical cooling range (CTR) The cooling tower Efficiency