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Sea level equation

The pressure of the atmosphere can be thought of as the pressure at the base of a column of fluid (air) located at the point of measurement (e.g., at sea level). Equation 3.4-1 can be used to calculate atmospheric pressure, assuming that the pressure at the top of the column (Pq) equals 0 and p and g are average values of the density of air and the acceleration of gravity between the top of the atmosphere and the measurement point. [Pg.56]

The e q>losion effects of a TNT charge are well documented as shown in Figure 3.3 for a hemispherical TNT surface charge at sea level. Equations for the functions in Figure 3.3 are provided in Table 3.1. The various explosion parameters in Figure 3.3 are correlated as a function of die scaled range, Z. The scaled... [Pg.135]

The maximum operation altitude of the above mentioned engine is 4.5 km from sea level. Equation (3.1) shows the relation between temperature, altitude and pressure. [Pg.42]

Schmidt P, Lund B, Naslund J-0, Fastook J (2014) Comparing a thermomechanical Weichselian Ice Sheet reconstruction to reconstructions based on the sea level equation aspects of ice configurations and glacial isostatic adjustment. Solid Earth 5 371-388. doi 10.5194/se-5-371-2014... [Pg.1779]

The theoretical steam rate (sometimes referred to as the water rate) for stream turbines can be determined from Keenan and Keyes or Mollier charts following a constant entropy path. The theoretical steam rate is given as Ib/hr/kw which is easily converted to Ib/hr/hp. One word of caution—in using Keenan and Keyes, steam pressures are given in PSIG. Sea level is the basis. For low steam pressures at high altitudes appropriate coirections must be made. See the section on Pressure Drop Air-Cooled Air Side Heat Exchangers, in this handbook, for the equation to correct atmospheric pressure for altitude. [Pg.126]

To obtain the governing minimum Q for the interval to be drilled. Equation 4-122 must be solved at 10,000 ft of depth. Since the drilling location is at a surface location of 6,000 ft above sea level, from Table 4-107, we have... [Pg.855]

It may not be well known that the weather bureau reports of barometric pressure are corrected to sea level even though describing conditions in the mountains, etc. Table IV gives the barometric pressure at various altitudes these should be used when applicable in equations 5 and 6. Representative cities and the variations in their respective altitudes are given in Table V. [Pg.163]

Liquid solvents in this picture may be considered as islands in the northern hemisphere, because the state of molecules in a liquid solvent is quite definitely closer to the COSMO state than to the vacuum. The only exception may be alkane solvents, which are located somewhere close to the equator due to their fully nonpolar character. Solids may be considered as sunken islands and their depths below sea level may be considered as AG s. As discussed before, the methods to explore this depth are rather limited, but we can be quite sure that in general the depth below sea level will be much smaller than the distance of the islands from the North Pole or from each other. We now explore the methods to go from the sea level position of any island to the North Pole or vice versa. Given such a method we will be able to transfer a compound from any liquid or supercooled liquid state to any other such state. [Pg.293]

T. cacao is cultivated at low altitudes within 1000 ft of sea level. Cacao grows exclusively between the latitudes 20°N and 20°S with 75% of the world s crop grown within 8° of the equator. Cacao requires a warm and humid climate and thrives best at shade temperatures of 65° to 95°F, although the tree has flourished under conditions of 105°F and almost 100% humidity found in areas of West Africa. Minimum rainfall requirements are an evenly distributed 40 in. per year with 60 to 80 in. desirable. [Pg.174]

A curve plotted from an equation in Ref. 12 is reproduced here as Figure 3. Above Ps = 100 psi and standard atmospheric conditions, Eq. (14) is increasingly in error compared to this curve, and should not be used. (Note that, at the surface of a spherical TNT charge at sea level,... [Pg.9]

This simple calculation shows why it is more difficult to breathe when up a mountain than at ground level the pressure term in Equation (8.18) decreases, so the rate at which oxygen enters the blood decreases in proportion to the decrease in the oxygen partial pressure. And the partial pressure is smaller at high altitudes than at sea level. [Pg.360]

The interval scale makes use of both the order and the distance characteristics of numbers but does not use the origin property. The origin of an interval scale is arbitrary. For instance, the zero point on the scale of elevation is arbitrarily set at sea level. Other interval scales are Celsius and Fahrenheit temperature, date, latitude, and exam scores. The origin of latitude, for example, is the equator. Because this... [Pg.17]

Evidence has been found that the place of origin is submerged land to the north west of New Guinea. The major coconut areas lie between 20°N and 20° S of the equator. Although it is found beyond this region, 27° N and 27° S, cultivation has not been successful and the palm does not fruit. Many varieties are found in Melanesian region. It is most widely cultivated in the tropics India, Ceylon, Malaysia, Indonesia, Philippines, South Sea Islands in the Pacific, East Africa, and Central and South Americas, up to 800 m above sea level, on humus-rich and porous soil or pure sand in coastal regions. [Pg.119]

The aqueous solubility of a gaseous compound is commonly reported for 1 bar (or 1 atm = 1.013 bar) partial pressure of the pure compound. One of the few exceptions is the solubility of 02 which is generally given for equilibrium with the gas at 0.21 bar, since this value is appropriate for the earth s atmosphere at sea level. As discussed in Chapter 3, the partial pressure of a compound in the gas phase (ideal gas) at equilibrium above a liquid solution is identical to the fugacity of the compound in the solution (see Fig. 3.9d). Therefore equating fugacity expressions for a compound in both the gas phase and an equilibrated aqueous solution phase, we have ... [Pg.139]

How much propane should a backpacker carry do we really need to carry a kilogram of gas Calculate the mass of propane that you would need to burn to obtain 350 kj of heat, which is just enough energy to heat 1 L of water from room temperature (20°C) to boiling at sea level (if we ignore all heat losses). The thermochemical equation is... [Pg.426]

The average proportion of water vapour at sea-level decreases in passing from the equator to the poles, so that each of the other constituents varies proportionally. J. Hann 6 gives for the average values ... [Pg.5]

The second approach to error assessment is a factor analysis of the various error sources within the procedure. These sources can be ascribed to the three major parameters in Equation (1) above vesicle size, hydrostatic pressure, and sea level atmospheric pressure. [Pg.206]

The radius of the Earth at the Equator is 6,378 km, so r in Equation 3.10 changes little as we move a short distance from the surface of the earth. The gravitational force is almost the same on top of Mt. Everest as it is at sea level. This lets us approximate the gravitational attraction to the Earth as ... [Pg.37]

The rise of atmospheric C02 with time is shown in Fig. 15.1. A prediction of the effects of this rise is more difficult. Preindustrial C02 concentration was 280 ppm (it was about 380 ppm at the century s end). Extrapolation of the present data to 2060 gives a doubling of the preindustrial concentration (560 ppm) and an associated temperature rise of 1.6 K at the equator. The corresponding estimated rise in sea level as a result of polar melting is 50 cm (see Fig. 15.3). Figure 15.4 shows the predicted temperature increases according to various assumptions. [Pg.480]

Meanwhile, the idea was formulated about resolving the full set of primitive hydro- and thermodynamic equations with all the boundary conditions specified successively correcting the current model fields of the temperature, salinity, and SLE by their observed values with the use of this or that kind of assimilation algorithm [35,36]. This approach is sometimes referred to as a four-dimensional analysis. Strictly speaking, it has little in common with the initial diagnostic methods. They are joined only by the common goal - the hydrodynamic calculations of the fields of currents from the data of observations of the temperature, salinity, and sea level. Therefore, in this section, we consider the results of application of all the above-mentioned approaches. [Pg.176]

Satellite altimeter observations were assimilated in two BSGC models 1.5-layer model with a reduced gravity acceleration [46] and in the slightly modified model [44,45] considered above. In the former model, the altimeter sea level was assimilated directly into the equations of continuity at each time step. In the latter model [47], the assimilation was similar to that in [44,45], where the differences between the model and observed temperature and salinity fields were retrieved from the level increments with the use of corresponding coefficients of proportionality. These coefficients depended on the depth and were determined from the relations between the SLE and the thermohaline fields obtained in [43] from the modeling results. Selected simplifications in the model physics helped to decrease the horizontal step of the grid in both of the calculations down to 7 km. [Pg.184]


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