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Simple Experiment Confirming the Negative Temperature Dependence of Gravity Force
SIMPLE EXPERIMENT CONFIRMING THE NEGATIVE TEMPERATURE DEPENDENCE OF GRAVITY FORCE Alexander L. Dmitriev St-Petersburg National Research University of Information Technologies, Mechanics and Optics, 49 Kronverksky Prospect, St-Petersburg, 197101, Russia Results of weighing of the tight vessel containing a thermo-isolated copper sample heated by a tungstic spiral are submitted. The increase of temperature of a sample with masse of 28 g for about 10 0 С causes a reduction of its apparent weight for 0.7 mg. The basic sources of measurement errors are briefly considered, the expediency of researches of temperature dependence of gravity is recognized. Key words: gravity force, weight, temperature, gravity mass. PACS: 04.80-y. Introduction The question on influence of temperature of bodies on the force of their gravitational interaction was already raised from the times when the law of gravitation was formulated. The first exact experiments in this area were carried out at the end of XIXth - the beginning of XXth century with the purpose of checking the consequences of various electromagnetic theories of gravitation (Mi, Weber, Morozov) according to which the force of a gravitational attraction of bodies is increased with the growth of their absolute temperature [1-3]. That period of experimental researches was completed in 1923 by the publication of Shaw and Davy’s work who concluded that the temperature dependence of gravitation forces does not exceed relative value of 2⋅10 −6 K −1 and can be is equal to zero [4]. Actually, as shown in [5], those authors confidently registered the negative temperature dependence of gravitation force. -
Weight and Lifestyle Inventory (Wali)
WEIGHT AND LIFESTYLE INVENTORY (Bariatric Surgery Version) © 2015 Thomas A. Wadden, Ph.D. and Gary D. Foster, Ph.D. 1 The Weight and Lifestyle Inventory (WALI) is designed to obtain information about your weight and dieting histories, your eating and exercise habits, and your relationships with family and friends. Please complete the questionnaire carefully and make your best guess when unsure of the answer. You will have an opportunity to review your answers with a member of our professional staff. Please allow 30-60 minutes to complete this questionnaire. Your answers will help us better identify problem areas and plan your treatment accordingly. The information you provide will become part of your medical record at Penn Medicine and may be shared with members of our treatment team. Thank you for taking the time to complete this questionnaire. SECTION A: IDENTIFYING INFORMATION ______________________________________________________________________________ 1 Name _________________________ __________ _______lbs. ________ft. ______inches 2 Date of Birth 3 Age 4 Weight 5 Height ______________________________________________________________________________ 6 Address ____________________ ________________________ ______________________/_______ yrs. 7 Phone: Cell 8 Phone: Home 9 Occupation/# of yrs. at job __________________________ 10 Today’s Date 11 Highest year of school completed: (Check one.) □ 6 □ 7 □ 8 □ 9 □ 10 □ 11 □ 12 □ 13 □ 14 □ 15 □ 16 □ Masters □ Doctorate Middle School High School College 12 Race (Check all that apply): □ American Indian □ Asian □ African American/Black □ Pacific Islander □White □ Other: ______________ 13 Are you Latino, Hispanic, or of Spanish origin? □ Yes □ No SECTION B: WEIGHT HISTORY 1. At what age were you first overweight by 10 lbs. or more? _______ yrs. old 2. What has been your highest weight after age 21? _______ lbs. -
Ideal Gasses Is Known As the Ideal Gas Law
ESCI 341 – Atmospheric Thermodynamics Lesson 4 –Ideal Gases References: An Introduction to Atmospheric Thermodynamics, Tsonis Introduction to Theoretical Meteorology, Hess Physical Chemistry (4th edition), Levine Thermodynamics and an Introduction to Thermostatistics, Callen IDEAL GASES An ideal gas is a gas with the following properties: There are no intermolecular forces, except during collisions. All collisions are elastic. The individual gas molecules have no volume (they behave like point masses). The equation of state for ideal gasses is known as the ideal gas law. The ideal gas law was discovered empirically, but can also be derived theoretically. The form we are most familiar with, pV nRT . Ideal Gas Law (1) R has a value of 8.3145 J-mol1-K1, and n is the number of moles (not molecules). A true ideal gas would be monatomic, meaning each molecule is comprised of a single atom. Real gasses in the atmosphere, such as O2 and N2, are diatomic, and some gasses such as CO2 and O3 are triatomic. Real atmospheric gasses have rotational and vibrational kinetic energy, in addition to translational kinetic energy. Even though the gasses that make up the atmosphere aren’t monatomic, they still closely obey the ideal gas law at the pressures and temperatures encountered in the atmosphere, so we can still use the ideal gas law. FORM OF IDEAL GAS LAW MOST USED BY METEOROLOGISTS In meteorology we use a modified form of the ideal gas law. We first divide (1) by volume to get n p RT . V we then multiply the RHS top and bottom by the molecular weight of the gas, M, to get Mn R p T . -
MAXIMUM METABOLISM FOOD METABOLISM PLAN the MAXIMUM Hreshold Spinach Salad: 1 Cup Spinach, 1/2 Cup Mixed 6 Oz
THE MAXIMUM METABOLISM FOOD PLAN™ WEEK ONE SUNDAY MONDAY TUESDAY WEDNESDAY THURSDAY FRIDAY SATURDAY Breakfast 3/4 oz. multi-grain cereal 1/2 cup oatmeal 2 lite pancakes (4” diameter); use non-stick 1 slice of wheat toast; top with 1/2 cup 1 1/2 oz. low fat granola Apple cinnamon crepe: 1 wheat tortilla, Omelet: 3 egg whites, 1 cup mixed zucchini, 1/2 sliced banana or 3/4 cup sliced 1/2 tbs. raisins pan; top with 1/2 cup peaches or 1/2 banana nonfat cottage cheese and 1/2 sliced 1 cup nonfat milk 1/3 cup nonfat ricotta cheese, 1 apple green peppers, onions, and tomatoes, 12 oz. of water before breakfast strawberries 1/2 cup nonfat milk 1 tbs. reduced calorie syrup apple; sprinkle with 1 tsp. cinnamon 1/2 medium banana (sliced), 1 tsp. cinnamon, 1/2 tsp. vanilla 2 oz. reduced calorie cheese, and salsa 1/2 cup nonfat milk 1 medium apple 1/2 cup low fat maple yogurt extract; heat in skillet over low flame 1 slice wheat toast 1/2 cup nonfat milk 1 tsp. butter Mid-Morning Snack 12 oz. water 12 oz. water 12 oz. water 12 oz. water 12 oz. water 12 oz. water 12 oz. water 1/2 bagel 1/2 cup nonfat yogurt 1/2 cup low fat cottage cheese 1 cup nonfat flavored yogurt with 1 tsp. 1 cup flavored nonfat yogurt 1 cup flavored nonfat yogurt 1 cup flavored nonfat yogurt 1 tbs. nonfat cream cheese 1/2 cup pineapple chunks sliced almonds 1 tbs. -
The Relation of Metabolic Rate to Body Weight and Organ Size
Pediat.Res. 1: 185-195 (1967) Metabolism basal metabolic rate growth REVIEW kidney glomerular filtration rate body surface area body weight oxygen consumption organ growth The Relation of Metabolic Rate to Body Weight and Organ Size A Review M.A. HOLLIDAY[54J, D. POTTER, A.JARRAH and S.BEARG Department of Pediatrics, University of California, San Francisco Medical Center, San Francisco, California, and the Children's Hospital Medical Center, Oakland, California, USA Introduction Historical Background The relation of metabolic rate to body size has been a The measurement of metabolic rate was first achieved subject of continuing interest to physicians, especially by LAVOISIER in 1780. By 1839 enough measurements pediatricians. It has been learned that many quanti- had been accumulated among subjects of different tative functions vary during growth in relation to sizes that it was suggested in a paper read before the metabolic rate, rather than body size. Examples of Royal Academy of France (co-authored by a professor these are cardiac output, glomerular filtration rate, of mathematics and a professor of medicine and oxygen consumption and drug dose. This phenomenon science) that BMR did not increase as body weight may reflect a direct cause and effect relation or may be increased but, rather, as surface area increased [42]. a fortuitous parallel between the relatively slower in- In 1889, RICHET [38] observed that BMR/kg in rab- crease in metabolic rate compared to body size and the bits of varying size decreased as body weight increased; function in question. RUBNER [41] made a similar observation in dogs. Both The fact that a decrease in metabolism and many noted that relating BMR to surface area provided re- other measures of physiological function in relation to a sults that did not vary significantly with size. -
Chapter 28 Pressure in Fluids
CHAPTER 28 PRESSURE IN FLUIDS EXERCISE 128, Page 281 1. A force of 280 N is applied to a piston of a hydraulic system of cross-sectional area 0.010 m 2 . Determine the pressure produced by the piston in the hydraulic fluid. force 280 N Pressure, p = = 28000Pa = 28 kPa area 0.010m2 That is, the pressure produced by the piston is 28 kPa 2. Find the force on the piston of question 1 to produce a pressure of 450 kPa. Pressure, p = 450 kPa = 450000 Pa force Pressure p = hence, force = pressure × area area = 4540000 × 0.010 = 4500 N = 4.5 kN 3. If the area of the piston in question 1 is halved and the force applied is 280 N, determine the new pressure in the hydraulic fluid. 0.010 New area = 0.005m2 2 force 280 N New pressure, p = = 56000Pa = 56 kPa area 0.005m2 331 © John Bird Published by Taylor and Francis EXERCISE 129, Page 283 1. Determine the pressure acting at the base of a dam, when the surface of the water is 35 m above base level. Take the density of water as 1000 kg/m 3 . Take the gravitational acceleration as 9.8 m/s 2 . Pressure at base of dam, p = gh = 1000 kg/m 3 9.8 m/s2 0.35 m = 343000 Pa = 343 kPa 2. An uncorked bottle is full of sea water of density 1030 kg/m 3 . Calculate, correct to 3 significant figures, the pressures on the side wall of the bottle at depths of (a) 30 mm, and (b) 70 mm below the top of the bottle. -
11 Archimedes Principle
Exp 11-1 P Experiment 11. Archimedes' Principle An application of Archimedes' principle - a piece of iron - sinks while a steel cup of the same weight floats on water. Objective: (a) To determine the specific gravity of a liquid by using a hydrometer. (b) the specific gravity of a solid heavier than water, the specific gravity of a liquid and the specific gravity of a solid lighter than water by· apj51yThg___Arcn1medes' principle: -- ····------···· --·-···- Apparatus: A balance, a solid heavier than water, a wooden cylinder, a hydrometer, alcohol and distilled water Theory: According to Archimedes' principle, when a body is immersed in a fluid (Fig. 1 ), either wholly or partially, the fluid exerts a buoyant force 8 on it. This buoyant force is equal to the weight of the fluid displaced by the body. Thus the apparent weight of the body is less than its actual weight, the loss of weight being equal to the buoyant force. - W = weight of the body B = buoyant force T = tension in the string supporting the body Fig. 1 Fig. 2 Consider the following problem: Weight of the body in air (actual weight of the body), w = 600 gm-wt Volume of the body, V = 80 cm3 Density of the liquid, p = 1.2 gm/cm 3 Volume of the liquid displaced = volume of the bodyVe = 80 cm3 Weight of the liquid displaced, we= Vex p = 96 gm-wt Buoyant force, B = 96 gm-wt Apparent weight of the body, wa = 600 - 96 gm-wt = 504 gm-wt Note that the apparent loss of weight of the body is equal to the - buoyant force of the fluid acting on the body, which, in turn, is equal to Exp 11-2P the weight of the flui9 displaced by the body. -
View the August Table of Excluded Times Due to Low Tides
WHATCOM COUNTY Ferry Department PUBLIC WORKS DEPARTMENT 322 N. Commercial Street, Suite 210 Bellingham, WA 98225-4042 JON HUTCHINGS Telephone: (360) 778-6200 DIRECTOR FAX: (360) 778-6201 www.whatcomcounty.us July 30, 2020 To Whom It May Concern: Re: Lummi Island Ferry Use Due to the damage we have incurred during low tides on the loading ramps at both Gooseberry Point and Lummi Island, we have had to find a solution to alleviate this problem. The ensuing policy was recommended by the Whatcom County Public Works Engineering Division, was reviewed by the County, and this policy was implemented effective May 22, 1995. NO TRUCK OVER 40,000 GVW WILL BE PERMITTED ON THE FERRY AT ANY TIDE UNDER ZERO The following timetable should assist you in scheduling deliveries to Lummi Island; however, should you have any questions regarding this timetable, please do not hesitate to contact the Whatcom Chief Ferry at (360) 815-5629. If you would like to be put on our Tide Table mailing list please contact Public Works Administration at (360) 778-6200 or email [email protected]. All times are acceptable, except as noted in the following tide timetable. AUGUST: 1 Between the hours of 8:10 a.m. - 12:15 p.m. excluded. 2 Between the hours of 8:55 a.m. - 1:00 p.m. excluded. 3 Between the hours of 9:45 a.m. - 1:30 p.m. excluded. 4 Between the hours of 10:30 a.m. - 1:55 p.m. excluded. 5 Between the hours of 11:30 a.m. -
12. Methods of Surface Tension Measurements
12. Methods of surface tension measurements There are several methods of surface tension measurements: 1. Capillary rise method 2. Stallagmometer method – drop weight method 3. Wilhelmy plate or ring method 4. Maximum bulk pressure method. 5. Methods analyzing shape of the hanging liquid drop or gas bubble. 6. Dynamic methods. 1. Capillary rise method This is the oldest method used for surface tension determination. A consequence of the surface tension appearance at the liquid/gas interface is moving up of the liquid into a thin tube, that is capillary, which is usually made of glass. This phenomenon was applied for determination of the liquid surface tension. For this purpose, a thin circular capillary is dipped into the tested liquid. If the interaction forces of the liquid with the capillary walls (adhesion) are stronger than those between the liquid molecules (cohesion), the liquid wets the walls and rises in the capillary to a defined level and the meniscus is hemispherically concave. In the opposite situation the forces cause decrease of the liquid level in the capillary below that in the chamber and the meniscus is semispherically convex. Both cases are illustrated in Fig. 11.1 Fig. 12.1. Schematic representation of the capillary rise method. If the cross-section area of the capillary is circular and its radius is sufficiently small, then the meniscus is semispherical. Along the perimeter of the meniscus there acts a force due to the surface tension presence. (1) f1 = 2π r γ cos θ Where: r – the capillary radius, γγγ – the liquid surface tension, θθθ – the wetting contact angle. -
Experiment 12 Archimedes' Principle
Experiment 12 Archimedes’ Principle Fig. 12-1 Equipment Graduated cylinder Triple Beam balance Pipette Wood cylinder Vernier caliper 2 Metal cylinders Rod & Clamp String Overflow container Experiment 12 Archimedes’ Principle Advance Reading: Serway & Jewett - Chapter 14, Section 14-4 Objective: The objective of this lab is to measure the buoyant force on a number of objects. Theory: Archimedes’ principle states that a body wholly or partially submerged in a fluid is buoyed up by a force equal in magnitude to the weight of the fluid displaced by the body. It is important to remember that fluid includes liquids and gases. This force is given by: FB = ρVg (Eq 1) where ρ (rho) is the density of the fluid, V is the volume of fluid displaced and g is acceleration due to gravity. It is the buoyant force that keeps ships afloat in water and hot air balloons floating in air. In this experiment, the buoyant force will be measured three ways and the results compared. The first method is by the measurement of force. This method involves weighing an object first in air, then in water, and using the difference in weight as the buoyant force. Though the object's mass does not change, its apparent weight will change when measured while immersed in a fluid that is denser than air. The second method is the displaced volume method. The volume of fluid displaced by the object is measured and its weight calculated. The weight of the water displaced is equal to the buoyant force exerted on the object, by Archimedes' Principle. -
2001: a Space Odyssey by James Verniere “The a List: the National Society of Film Critics’ 100 Essential Films,” 2002
2001: A Space Odyssey By James Verniere “The A List: The National Society of Film Critics’ 100 Essential Films,” 2002 Reprinted by permission of the author Screwing with audiences’ heads was Stan- ley Kubrick’s favorite outside of chess, which is just another way of screwing with heads. One of the flaws of “Eyes Wide Shut” (1999), Kubrick’s posthumously re- leased, valedictory film, may be that it doesn’t screw with our heads enough. 2001: A Space Odyssey (1968), however, remains Kubrick’s crowning, confounding achievement. Homeric sci-fi film, concep- tual artwork, and dopeheads’ intergalactic Gary Lockwood and Keir Dullea try to hold a discussion away from the eyes of HAL 9000. joyride, 2001 pushed the envelope of film at Courtesy Library of Congress a time when “Mary Poppins” and “The Sound of Music” ruled the box office. 3 million years in the past and ends in the eponymous 2001 with a sequence dubbed, with a wink and nod to As technological achievement, it was a quantum leap be- the Age of Aquarius, “the ultimate trip.” In between, yond Flash Gordon and Buck Rogers serials, although it “2001: A Space Odyssey” may be more of a series of used many of the same fundamental techniques. Steven landmark sequences than a fully coherent or satisfying Spielberg called 2001 “the Big Bang” of his filmmaking experience. But its landmarks have withstood the test of generation. It was the precursor to Andrei Tarkovsky’s time and repeated parody. “Solari” (1972), Spielberg’s “Close Encounters of the Third Kind” (1977) and George Lucas’s “Star The first arrives in the wordless “Dawn of Man” episode, Wars” (1977), as well as the current digital revolution. -
43759498.Pdf
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Keele Research Repository This work is protected by copyright and other intellectual property rights and duplication or sale of all or part is not permitted, except that material may be duplicated by you for research, private study, criticism/review or educational purposes. Electronic or print copies are for your own personal, non- commercial use and shall not be passed to any other individual. No quotation may be published without proper acknowledgement. For any other use, or to quote extensively from the work, permission must be obtained from the copyright holder/s. The security of the European Union’s critical outer space infrastructures Phillip A. Slann This electronic version of the thesis has been edited solely to ensure compliance with copyright legislation and excluded material is referenced in the text. The full, final, examined and awarded version of the thesis is available for consultation in hard copy via the University Library Thesis submitted for the degree of Doctor of Philosophy in International Relations March 2015 Keele University Abstract This thesis investigates the European Union’s (EU) conceptualisation of outer space security in the absence of clear borders or boundaries. In doing so, it analyses the means the EU undertakes to secure the space segments of its critical outer space infrastructures and the services they provide. The original contribution to knowledge offered by this thesis is the framing of European outer space security as predicated upon anticipatory mechanisms targeted towards critical outer space infrastructures. The objective of this thesis is to contribute to astropolitical literature through an analysis of the EU’s efforts to secure the space segments of its critical outer space infrastructures, alongside a conceptualisation of outer space security based upon actor-specific threats, critical infrastructures and anticipatory security measures.