Chapter Two Properties of Ammonia
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Chapter 5 Measures of Humidity Phases of Water
Chapter 5 Atmospheric Moisture Measures of Humidity 1. Absolute humidity 2. Specific humidity 3. Actual vapor pressure 4. Saturation vapor pressure 5. Relative humidity 6. Dew point Phases of Water Water Vapor n o su ti b ra li o n m p io d a a at ep t v s o io e en s n d it n io o n c freezing Liquid Water Ice melting 1 Coexistence of Water & Vapor • Even below the boiling point, some water molecules leave the liquid (evaporation). • Similarly, some water molecules from the air enter the liquid (condense). • The behavior happens over ice too (sublimation and condensation). Saturation • If we cap the air over the water, then more and more water molecules will enter the air until saturation is reached. • At saturation there is a balance between the number of water molecules leaving the liquid and entering it. • Saturation can occur over ice too. Hydrologic Cycle 2 Air Parcel • Enclose a volume of air in an imaginary thin elastic container, which we will call an air parcel. • It contains oxygen, nitrogen, water vapor, and other molecules in the air. 1. Absolute Humidity Mass of water vapor Absolute humidity = Volume of air The absolute humidity changes with the volume of the parcel, which can change with temperature or pressure. 2. Specific Humidity Mass of water vapor Specific humidity = Total mass of air The specific humidity does not change with parcel volume. 3 Specific Humidity vs. Latitude • The highest specific humidities are observed in the tropics and the lowest values in the polar regions. -
Physics, Chapter 17: the Phases of Matter
University of Nebraska - Lincoln DigitalCommons@University of Nebraska - Lincoln Robert Katz Publications Research Papers in Physics and Astronomy 1-1958 Physics, Chapter 17: The Phases of Matter Henry Semat City College of New York Robert Katz University of Nebraska-Lincoln, [email protected] Follow this and additional works at: https://digitalcommons.unl.edu/physicskatz Part of the Physics Commons Semat, Henry and Katz, Robert, "Physics, Chapter 17: The Phases of Matter" (1958). Robert Katz Publications. 165. https://digitalcommons.unl.edu/physicskatz/165 This Article is brought to you for free and open access by the Research Papers in Physics and Astronomy at DigitalCommons@University of Nebraska - Lincoln. It has been accepted for inclusion in Robert Katz Publications by an authorized administrator of DigitalCommons@University of Nebraska - Lincoln. 17 The Phases of Matter 17-1 Phases of a Substance A substance which has a definite chemical composition can exist in one or more phases, such as the vapor phase, the liquid phase, or the solid phase. When two or more such phases are in equilibrium at any given temperature and pressure, there are always surfaces of separation between the two phases. In the solid phase a pure substance generally exhibits a well-defined crystal structure in which the atoms or molecules of the substance are arranged in a repetitive lattice. Many substances are known to exist in several different solid phases at different conditions of temperature and pressure. These solid phases differ in their crystal structure. Thus ice is known to have six different solid phases, while sulphur has four different solid phases. -
Ammonia, Anhydrous Ama
AMMONIA, ANHYDROUS AMA CAUTIONARY RESPONSE INFORMATION 4. FIRE HAZARDS 7. SHIPPING INFORMATION 4.1 Flash Point: 7.1 Grades of Purity: Commercial, industrial, Common Synonyms Liquefied compressed Colorless Ammonia odor Not flammable under conditions likely to refrigeration, electronic, and metaflurgical Liquid ammonia gas be encountered grades all have purity greater than 99.5% 4.2 Flammable Limits in Air: 15.50%- 7.2 Storage Temperature: Ambient for pressurized 27.00% ammonia; low temperature for ammonia at Floats and boils on water. Poisonous, visible vapor cloud is produced. 4.3 Fire Extinguishing Agents: Stop flow of atmospheric pressure Avoid contact with liquid and vapor. Keep people away. gas or liquid. Let fire burn. 7.3 Inert Atmosphere: No requirement Wear goggles, self-contained breathing apparatus, and rubber overclothing (including gloves). 4.4 Fire Extinguishing Agents Not to Be 7.4 Venting: Safety relief 250 psi for ammonia Stop discharge if possible. Used: None under pressure. Pressure-vacuum for Stay upwind and use water spray to ``knock down'' vapor. 4.5 Special Hazards of Combustion ammonia at atmospheric pressure. Call fire department. Products: Not pertinent Isolate and remove discharged material. 7.5 IMO Pollution Category: Currently not available 4.6 Behavior in Fire: Not pertinent Notify local health and pollution control agencies. 7.6 Ship Type: 2 4.7 Auto Ignition Temperature: 1204°F Protect water intakes. 7.7 Barge Hull Type: 2 4.8 Electrical Hazards: Class I, Group D Combustible. 4.9 Burning Rate: 1 mm/min. Fire 8. HAZARD CLASSIFICATIONS Wear goggles, self-contained breathing apparatus, and rubber over- 4.10 Adiabatic Flame Temperature: Currently clothing (including gloves). -
HEATS of COMBUSTION of DIAMOND and of GRAPHITE by Ralph S
r---------------___........,._ . _____~ ~_ U. S. DEPARTMENT OF COMMERCE NATIONAL BUREAU OF STANDARDS RESEARCH PAPER RP1140 Part of Journal of Research of the }.{ational Bureau of Standards, Volume 21, October 1938 HEATS OF COMBUSTION OF DIAMOND AND OF GRAPHITE By Ralph S. Jessup ABSTRACT Measurements were made of the heats of combustion of one artificial graphite, two natural graphites, and two samples of diamond. The bomb calorimeter used was calibrated electrically and by means of benzoic acid. The amount of reaction in each combustion experiment was determined from the mass of carbon dioxide formed. This method of determining the amount of reaction automatically eliminates the effect of unburned carbon and of some impurities. It was found, however, that results for different samples did not agree unless the samples were purified. Two methods of purification were used: (a) heating in vacuo to 1,800° C and (b) treatment with hydrochloric and hydrofluoric acids and subsequent heating in vacuo to 200° C to remove traces of the acids. Both methods yielded graphite containing only small amounts of impurities. The mean value obtained for the heat of combustion (-/lH) of the purified graphites in oxygen at 25° C and a constant pressure of 1 atmosphere to form gaseous carbon dioxide at the same temperature and pressure was 393.396 international kilojoules per mole (44.010 g of CO2). The maximum deviation of the mean value for anyone of the purified samples from this value was 0.021 percent. The two samples of diamond, purified by treatment with aqueous hydrochloric and hydrofluoric acids and subsequently heated in vacuo to about 570° C, had average particle sizes of 2.5 I'- and 39.5 1'-, respectively, and yielded the following respective mean values for the heat of combustion (-/lH) at 25° C and 1 atmos phere, in oxygen to form gaseous carbon dioxide: 395.771 and 395.287 interna tional kilojoules per mole. -
Pressure Vs Temperature (Boiling Point)
Boiling Points and Vapor Pressure Background Boiling Points and Vapor Pressure Background: Definitions Vapor Pressure: The equilibrium pressure of a vapor above its liquid; the pressure of the vapor resulting from the evaporation of a liquid above a sample of the liquid in a closed container. Boiling Point: The temperature at which the vapor pressure of a liquid is equal to the atmospheric (or applied) pressure. As the temperature of the liquid increases, the vapor pressure will increase, as seen below: https://www.chem.purdue.edu/gchelp/liquids/vpress.html Vapor pressure is interpreted in terms of molecules of liquid converting to the gaseous phase and escaping into the empty space above the liquid. In order for the molecules to escape, the intermolecular forces (Van der Waals, dipole- dipole, and hydrogen bonding) have to be overcome, which requires energy. This energy can come in the form of heat, aka increase in temperature. Due to this relationship between vapor pressure and temperature, the boiling point of a liquid decreases as the atmospheric pressure decreases since there is more room above the liquid for molecules to escape into at lower pressure. The graph below illustrates this relationship using common solvents and some terpenes: Pressure vs Temperature (boiling point) Ethanol Heptane Isopropyl Alcohol B-myrcene 290.0 B-caryophyllene d-Limonene Linalool Pulegone 270.0 250.0 1,8-cineole (eucalyptol) a-pinene a-terpineol terpineol-4-ol 230.0 p-cymene 210.0 190.0 170.0 150.0 130.0 110.0 90.0 Temperature (˚C) Temperature 70.0 50.0 30.0 10 20 30 40 50 60 70 80 90 100 200 300 400 500 600 760 10.0 -10.0 -30.0 Pressure (torr) 1 Boiling Points and Vapor Pressure Background As a very general rule of thumb, the boiling point of many liquids will drop about 0.5˚C for a 10mmHg decrease in pressure when operating in the region of 760 mmHg (atmospheric pressure). -
ESSENTIALS of METEOROLOGY (7Th Ed.) GLOSSARY
ESSENTIALS OF METEOROLOGY (7th ed.) GLOSSARY Chapter 1 Aerosols Tiny suspended solid particles (dust, smoke, etc.) or liquid droplets that enter the atmosphere from either natural or human (anthropogenic) sources, such as the burning of fossil fuels. Sulfur-containing fossil fuels, such as coal, produce sulfate aerosols. Air density The ratio of the mass of a substance to the volume occupied by it. Air density is usually expressed as g/cm3 or kg/m3. Also See Density. Air pressure The pressure exerted by the mass of air above a given point, usually expressed in millibars (mb), inches of (atmospheric mercury (Hg) or in hectopascals (hPa). pressure) Atmosphere The envelope of gases that surround a planet and are held to it by the planet's gravitational attraction. The earth's atmosphere is mainly nitrogen and oxygen. Carbon dioxide (CO2) A colorless, odorless gas whose concentration is about 0.039 percent (390 ppm) in a volume of air near sea level. It is a selective absorber of infrared radiation and, consequently, it is important in the earth's atmospheric greenhouse effect. Solid CO2 is called dry ice. Climate The accumulation of daily and seasonal weather events over a long period of time. Front The transition zone between two distinct air masses. Hurricane A tropical cyclone having winds in excess of 64 knots (74 mi/hr). Ionosphere An electrified region of the upper atmosphere where fairly large concentrations of ions and free electrons exist. Lapse rate The rate at which an atmospheric variable (usually temperature) decreases with height. (See Environmental lapse rate.) Mesosphere The atmospheric layer between the stratosphere and the thermosphere. -
Thermochemistry of Heteroatomic Compounds:Calculation of the Heat
Open Journal of Physical Chemistry, 2011, 1, 1-5 doi:10.4236/ojpc.2011.11001 Published Online May 2011 (http://www.SciRP.org/journal/ojpc) Thermochemistry of Heteroatomic Compounds: Calculation of the heat of Combustion and the heat of Formation of some Bioorganic Molecules with Different Hydrophenanthrene Rows Vitaly V. Ovchinnikov Tupolev Kazan State Technical University, St- K. Marks 10, 420111 Kazan, Russian Federation E-mail: [email protected] Received March 23rd, 2011; revised April 10th, 2011; accepted May 10th, 2011. Abstract On the basis of the known experimental heats of combustions of the seventeen alkanes in condensed state, the general equation comb HifNg has been deduced, in which i and f are correlation coefficients, N and g are a numbers of valence electrons and lone electron pairs of heteroatoms in molecule. The pre- sented dependence has been used for the calculation of the heats of combustion of thirteen organic molecules with biochemical properties: holestan, cholesterol, methyl-cholesterol, ergosterol, vitamin-D2, estradiol, an- drostenone, testosterone, androstanedione, morphine, morphinanone, codeine and pentasozine. It is noted that good convergence was obtained within the limits of errors of thermochemical experiments known in the literature and calculations of the heats of combustion for some of them were conducted. With the application of Hess law and the heats of vaporization vap H , which has been calculated with the use of a topological 1 s solvation index of the first order x , the heats of formation f H for condensed and gaseous phases were calculated for the listed bioorganic molecules. Keywords: Alkanes, Biochemical Molecules, the Heat of Combustion, Heat of Formation, Heat of Vaporiza- tion, Topological Solvation Index 1. -
Problem Set #10 Assigned November 8, 2013 – Due Friday, November 15, 2013 Please Show All Work for Credit
Problem Set #10 Assigned November 8, 2013 – Due Friday, November 15, 2013 Please show all work for credit To Hand in 1. 1 2. –1 A least squares fit of ln P versus 1/T gives the result Hvaporization = 25.28 kJ mol . 3. Assuming constant pressure and temperature, and that the surface area of the protein is reduced by 25% due to the hydrophobic interaction: 2 G 0.25 N A 4 r Convert to per mole, ↓determine size per molecule 4 r 3 V M N 0.73mL/ g 60000g / mol (6.02 1023) 3 2 2 A r 2.52 109 m 2 23 9 2 G 0.25 N A 4 r 0.0720N / m 0.25 6.02 10 / mol (4 ) (2.52 10 m) 865kJ / mol We think this is a reasonable approach, but the value seems high 2 4. The vapor pressure of an unknown solid is approximately given by ln(P/Torr) = 22.413 – 2035(K/T), and the vapor pressure of the liquid phase of the same substance is approximately given by ln(P/Torr) = 18.352 – 1736(K/T). a. Calculate Hvaporization and Hsublimation. b. Calculate Hfusion. c. Calculate the triple point temperature and pressure. a) Calculate Hvaporization and Hsublimation. From Equation (8.16) dPln H sublimation dT RT 2 dln P d ln P dT d ln P H T 2 sublimation 11 dT dT R dd TT For this specific case H sublimation 2035 H 16.92 103 J mol –1 R sublimation Following the same proedure as above, H vaporization 1736 H 14.43 103 J mol –1 R vaporization b. -
Thermal Properties of Petroleum Products
UNITED STATES DEPARTMENT OF COMMERCE BUREAU OF STANDARDS THERMAL PROPERTIES OF PETROLEUM PRODUCTS MISCELLANEOUS PUBLICATION OF THE BUREAU OF STANDARDS, No. 97 UNITED STATES DEPARTMENT OF COMMERCE R. P. LAMONT, Secretary BUREAU OF STANDARDS GEORGE K. BURGESS, Director MISCELLANEOUS PUBLICATION No. 97 THERMAL PROPERTIES OF PETROLEUM PRODUCTS NOVEMBER 9, 1929 UNITED STATES GOVERNMENT PRINTING OFFICE WASHINGTON : 1929 F<ir isale by tfttf^uperintendent of Dotmrtients, Washington, D. C. - - - Price IS cants THERMAL PROPERTIES OF PETROLEUM PRODUCTS By C. S. Cragoe ABSTRACT Various thermal properties of petroleum products are given in numerous tables which embody the results of a critical study of the data in the literature, together with unpublished data obtained at the Bureau of Standards. The tables contain what appear to be the most reliable values at present available. The experimental basis for each table, and the agreement of the tabulated values with experimental results, are given. Accompanying each table is a statement regarding the esti- mated accuracy of the data and a practical example of the use of the data. The tables have been prepared in forms convenient for use in engineering. CONTENTS Page I. Introduction 1 II. Fundamental units and constants 2 III. Thermal expansion t 4 1. Thermal expansion of petroleum asphalts and fluxes 6 2. Thermal expansion of volatile petroleum liquids 8 3. Thermal expansion of gasoline-benzol mixtures 10 IV. Heats of combustion : 14 1. Heats of combustion of crude oils, fuel oils, and kerosenes 16 2. Heats of combustion of volatile petroleum products 18 3. Heats of combustion of gasoline-benzol mixtures 20 V. -
1 Volumetric Energy Density of Compressed Air and Compressed
Volumetric Energy Density of Compressed Air and Compressed Methane. Volumetric energy density is a combination of the potential for mechanical work, w, done by the change in pressure (P), and volume (V), and the chemical heat, q, released from burning the gas. For example, compressed air at 2,900 psi (~197 atm) has an energy density of 0.1 MJ/L calculated from PV and compressed methane (at 2,900 psi) has an energy density of 8.0 MJ/L calculated from the combination of PV and heat of combustion (Eq. 1). Estimate of Pressure Immediately After Ignition. Using the unpressurized channel volume of 1.0 mL, and our theoretically estimated temperature immediately after ignition of 2,800 oC, we calculated the maximum pressure, using the ideal gas law, to be ~1 MPa (~140 psi). Though this value is an overestimate (it does not take into account the channel volume expansion and the gas cooling, a complex calculation that is beyond the scope of this paper), we use it to illustrate the quick impulse of high pressure to use a passive valving system to control the flow of gas out of the channel after combustion and cooling. Fabrication of the Robot. The elastomer we used for the actuation layer was a stiff silicone rubber (Dragon Skin 10, DS-10; Smooth-on, Inc.). This elastomer has a greater Young’s modulus than our previous choice for pneumatic actuation (Ecoflex 00-30; Smooth-on, Inc.); pneu-nets composed of DS-10 could withstand the large forces generated within the channels during the explosion better than Ecoflex; in addition, DS-10 has a high resilience, which allowed the pneu-nets to release stored elastic energy rapidly for propulsion (Fig. -
The Thermodynamic Properties of Nitrogen from 64 to 300* K Between
Lonal Bureau of btaudaj a.^ Lilarary, M.W. Bldg JUIV 6 1962 PB 161630 ^ecknlcciL ^^ote 129 THE THERMODYNAMIC PROPERTIES OF NITROGEN FROM 64 TO 300^ K BETWEEN 0.1 AND 200 ATMOSPHERES THOMAS R. STROBRIDGE U. S. DEPARTMENT OF COMMERCE NATIONAL BUREAU OF STANDARDS THE NATIONAL BUREAU OF STANDARDS Functions and Activities The functions of the National Bureau of Standards are set forth in the Act of Congress, March 3, 1901, as amended by Congress in Public Law 619, 1950. These include the development and maintenance of the na- tional standards of measurement and the provision of means and methods for making measurements consistent with these standards; the determination of physical constants and properties of materials; the development of methods and instruments for testing materials,- devices, and structures; advisory services to government agen- cies on scientific and technical problems; invention and development of devices to serve special needs of the Government; and the development of standard practices, codes, and specifications. The work includes basic and applied research, development, engineering, instrumentation, testing, evaluation, calibration services, and various consultation and information services. Reseeirch projects are also performed for other government agencies when the work relates to and supplements the basic program of the Bureau or when the Bureau's unique competence is required. The scope of activities is suggested by the listing of divisions and sections on the inside of the back cover. Publications The results of the Bureau's research are published either in the Bureau's own series of publications or in the journals of professional and scientific societies. -
Aqua Ammonia Customer Manual
CUSTOMER MANUAL – AQUA AMMONIA TABLE OF CONTENTS AQUA AMMONIA PROPERTIES. 2 AQUA AMMONIA QUALITY . 3 HAZARDOUS PROPERTIES . ... 4 AQUA AMMONIA – STRENGTH DETERMINATION. .. 4 SHIPPING CONTAINERS FOR AQUA AMMONIA . 5 STORAGE OF AQUA AMMONIA . 6 AQUA AMMONIA STORAGE TANKS . 6 BULK DELIVERIES BY CARGO TANKS . 6 MATERIALS FOR PIPING & FITTINGS . .. 7 SYSTEM DESIGN . .. 8 AQUA AMMONIA TRANSFER METHODS DRAWING # 8031 . 9 Page 1 Revision 5/98 LEGAL NOTICE: Copyright © 1998 Tanner Industries, Inc. (“TII”). This document is provided for use by customers and prospective customers of TII only. This document may not be modified, distributed, or reproduced in any form, or by any electronic or mechanical means, including the use of information storage and retrieval systems, without permission in writing from TII. All rights reserved. Unauthorized use is strictly prohibited. AQUA AMMONIA PROPERTIES Aqua ammonia, also called ammoniacal liquor, ammonia liquor or ammonia water is produced by dissolving ammonia gas in water. Its proper chemical name is Ammonium Hydroxide. The grades, or strength of Ammonium Hydroxide usually available commercially are 26° and 21° Baumé. However, Tanner Industries can produce any strength to meet our customers requirements. The Baumé reading refers to a specific gravity scale. A 26° Baumé solution is equivalent to 29.4% and 21° Baumé solution is equivalent to 19.68%, both by weight of ammonia dissolved in water. Since the Baumé reading varies with temperature, the reading is standardized at 60°F. The density of the material compared to water is 0.8974. See Aqua Ammonia Table. Aqua ammonia is corrosive to copper, cooper alloys, aluminum alloys and galvanized surfaces.