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Free fall acceleration

The weight of an object is the force exerted on the object by gravitational attraction. Suppose that an object of mass m is subjected to a gravitational force W (W is by definition the weight of the object) and that if this object were falling freely its acceleration would be g. The weight, mass, and free-fall acceleration of the object are related by Equation 2.4-4 ... [Pg.12]

Consider the gravitational constant gc- what is it We define Newton s second law by measuring the acceleration that one pound force imparts to one pound mass during free fall. We stipulate that free fall occurs at 45 degree latitude and at sea level. Free fall acceleration thus defined is 32 ft/s. Newton s second law, therefore, becomes... [Pg.26]

Figures 11.9 and 11.10 present the dependence of the relative length Ljd (L -flame length, d - nozzle diameter) of the turbulent flame on the Froude number Fr = U / gd), U - flow rate at the nozzle exit section, g - free fall acceleration. It is seen that in the low-Froude number region (less than 10 ), the experimental data are well described by the interpolated relation [24]... Figures 11.9 and 11.10 present the dependence of the relative length Ljd (L -flame length, d - nozzle diameter) of the turbulent flame on the Froude number Fr = U / gd), U - flow rate at the nozzle exit section, g - free fall acceleration. It is seen that in the low-Froude number region (less than 10 ), the experimental data are well described by the interpolated relation [24]...
Now we have to solve a problem of the many real reference systems we usually deal with, in practice, those that can be considered to be inertial. Many problems of mechanics are considered in a laboratory reference system, strictly bound to the surface of the earth. Is this reference system an inertial one Strictly speaking, the answer is no, since the earth rotates daily, the points on the terrestrial surface (excluding the poles) possess different acceleration, perpendicular to the axis of the earth s rotation. However, in comparison with free-falling acceleration, this acceleration is very small, and for practical problems connected with the earth in a laboratory system, it is possible to consider it to be inertial. [Pg.20]

Determine the relationship of the free fall acceleration g with a distance from the Earth s center r. Assume that the earth density p is a constant independent of the earth point. Draw a graph g(r). Assume the earth s radius R to be constant. [Pg.98]

Maxwell molecular velocity distribution molecule kinetic energy distribution free fall acceleration vector gyromagnetic ratio, Lande factor vector of magnetic field strength Planck s constant Miller indexes... [Pg.605]

V is the velocity of sedimentation and a is the acceleration of free fall or centrifugation. [Pg.84]

Fig. 23. Pressure drop and flooding correlation for various random packings (95). ip = p- o IP-l (standard acceleration of free fall) = 9.81 m/s, p, = liquid viscosity ia mPa-s numbers on lines represent pressure drop, mm H2O /m of packed height to convert to ia. H2O /ft multiply by 0.012. Packing... Fig. 23. Pressure drop and flooding correlation for various random packings (95). ip = p- o IP-l (standard acceleration of free fall) = 9.81 m/s, p, = liquid viscosity ia mPa-s numbers on lines represent pressure drop, mm H2O /m of packed height to convert to ia. H2O /ft multiply by 0.012. Packing...
Particles of different sizes fall at different velocities. When a set of different-sized particles falls in a group, the particles collide with each other and the faster ones tend to accelerate the slower ones. In all collisions the linear momentum is conserved, so that if all particles collide with each other sufficiently many times, the set of particles will achieve one mean free-falling velocity. Thus the mean free-falling velocity of the set of particles can be defined by... [Pg.1327]

We want to find the relation between the height, h, of the column of mercury in a barometer and the atmospheric pressure, P. Suppose the cross-sectional area of the column is A. The volume of mercury in the column is the height of the cylinder times this area, V = bA. The mass, ttt, of this volume of mercury is the product of mercury s density, d, and the volume so m = dV = dhA. The mercury is pulled down by the force of gravity and the total force that its mass exerts at its base is the product of the mass and the acceleration of free fall (the acceleration due to gravity), g F = mg. Therefore, the pressure at the base of the column, the force divided by the area, is... [Pg.263]

This pressure can also be reported as 101 kPa, where 1 kPa = 103 Pa. The acceleration of free fall varies over the surface of the Earth and depends on the altitude in all calculations in this text, we assume that g has the standard value used here. [Pg.264]

The height, h, of a column of liquid in a capillary tube can be estimated by using h = lylgdr, where y is the surface tension, d is the density of the liquid, g is the acceleration of free fall, and r is the radius of the tube. Which will rise higher in a tube that is 0.15 mm in diameter at 25°C, water or ethanol The density of water is 0.997 g-cm-3 and that of ethanol is 0.79 g-cm-3. See Table 5.3. [Pg.329]

FIGURE 834 The pressure at the base of a column of fluid is equal to the product of the acceleration of free fall, g, the density, d, of the liquid, and the height, h, of the column. [Pg.456]

In some cases, it may be necessary to calculate the osmotic pressure from the height, h, of the solution (in an apparatus like that in Fig. 8.31) by using 11 = gdh, where d is the density of the solution and g is the acceleration of free fall (see inside back cover). [Pg.457]


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Acceleration of free fall

Falling

Falls

Falls/falling

Free fall

Standard acceleration of free fall

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