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Pascal s law

Figure 40.2 illustrates the transmission of forces through liquids. For Pascal s law to become effective for practical applications, a piston or ram confined within a close tolerance cylinder was needed. It was not until the latter part of the eighteenth century that methods were developed that could make the snugly fitted parts required making hydraulic systems practical. [Pg.585]

Remember that Pascal s law states that a pressure set up in a fluid acts equally in all directions and at right angles... [Pg.591]

Review the system illustrated in Figure 40.8. Chamber A is under pressure and is connected by a tube to chamber B, which is also under pressure. The pressure in chamber A is static pressure of lOOpsi. The pressure at some point (X) along the connecting tube consists of a velocity pressure of lOpsi exerted in a direction parallel to the line of flow, plus the unused static pressure of 90psi. The static pressure (90psi) follows Pascal s law and exerts equal pressure in all directions. As the fluid enters chamber B, it slows down and its velocity is reduced. As a volume of liquid moves from a small, confined space into a larger area, the fluid will expand to fill the greater volume. The result of this expansion is a reduction of velocity and a momentary reduction in pressure. [Pg.592]

So far, we have explained the effects of atmospheric pressure on liquids and how external forces are distributed through liquids. Let us now focus our attention on forces generated by the weight of liquids themselves. To do this, we must first discuss density, specific gravity and Pascal s law. [Pg.593]

According to Pascal s law, any force applied to a confined fluid is transmitted uniformly in all directions throughout... [Pg.593]

At this point, you should note that since Pascal s law is independent of the shape of the container, it is not necessary that the tube connecting the two pistons has the same cross-sectional area of the pistons. A connection of any size, shape or length will do, as long as an unobstructed passage is provided. Therefore, the system shown in Figure 40.11, with a relatively small, bent pipe connecting two cylinders will act the same as the system shown in Figure 40.10. [Pg.593]

A pressure applied at any point on the boundary of a fluid is transmitted uniformly throughout the whole fluid (Pascal s law). [Pg.40]

Papin s digester, 177 Partial pressures, lawr of, 171, 265, 274 Pascal s law, 40 Passive resistances, 91 Path, 44... [Pg.542]

Pascal s law states that the pressure in a static fluid is the same in all directions. This condition is different from that for a stressed solid in static equilibrium. In such a solid, the stress on a plane depends upon the orientation of that plane, A liquid m contact with the atmosphere is sometimes called a free surface. A static liquid has a horizontal free surface if gravity is the only type of force acting. [Pg.1367]

For isotropic bulk phases at equilibrium, the pressure is a scalar and the same everywhere. This is Pascal s law. In Inhomogeneous systems, like interfaces, this is no longer true. Then, very generally, the pressure acquires tensorlal nature, characterized by nine components. [Pg.134]

Now, it is well known that in the inn r part of a fluid the pressure across a plane is the same irrespective of the directions of the plane, that is, Pascal s law holds. But Eq. II.1 shows that surface tension arises from the circumstance that the law does not hold in the transition region of two homogeneous phases. Thus the pressure pr (tangential pressure) across a plane perpendicular to the surface of the liquid is different from that across a plane parallel to the surface of the liquid. The latter may be called the normal pressure and denoted by />N. Since />N is shown to have the same value irrespective of position, it may be denoted simply by p as is done in Eq. II.l... [Pg.206]

It is well known that Pascal s law holds in a fluid in which the stress across any elementary plane is perpendicular to the plane. In the transition layer, where the density changes from the value for bulk liquid to the value for gaseous state in traversing a layer of atomic dimension, Pascal s law does not hold, and the stress across a strip parallel to the boundary is different from that across a strip perpendicular to the boundary. [Pg.220]

The definition of a invariant with respect to positioning of the dividing surface can be worked out, if one analyzes trends in the/z)-pc(z) function within the discontinuity surface. The specified quantity has the same value in the bulk of both phases, equal to the negative external pressure (Fig. 1-4). Within the discontinuity surface, pressure p has a tensor nature, making Pascal s law invalid. Meanwhile, the concentration and pressure dependence of the surface energy density,/ given by eq. (1.1), is valid only in the regions where Pascal s law holds, i.e., where pressure is a scalar quantity (direct summation of a scalar and a tensor within the same equation is not permitted). [Pg.8]

PASCAL S LAW - Pressure imposed upon a fluid is transmitted equally in all directions. [Pg.112]

Woemly (1955) determined the magnetic susceptibility of a-tocopherol as X = —0.773 X 10 , a value which agrees perfectly with that calculated according to Pascal s law (x = —0.774 X 10 ). [Pg.419]

Pascal s law states that for a fluid at rest, pressure at a point is the same in all directions. Note carefully that we are discussing pressure at a point. To demonstrate this law, consider the vessel shown in Figure 10.9j the pressure at pointy is the same in all directions. [Pg.246]

You should undersmnd what is meant by pressure. For stadc fluids, you diould understand Pascal s law, which states that fluid pressure at a point is the same in all direcdons. You should also remember the reladonship between the fluid pressure and the dq>th of the fluicL You should undemand what the fluid properdes such as viscosity and bulk modulus of compressibility mean. You should also have a good idea of how hydraulic systems work. [Pg.271]

Pascal s law Pascal s law states that when there is an increase in pressure at any point in a confined fluid, there is an equal increase at every other point in the container. [Pg.237]

We can apply Pascal s law througji basic mathematics. In Figure 11-11, 250 pounds are being apphed to piston A. The resulting... [Pg.237]

Engineers use Pascal s law to assist with the design process. Before fabricating prototypes, engineers use math to determine a solution for their design problems. [Pg.239]

ENGINEERING CHALLENGE 1 Applying Boyle s, Charles s, and Pascal s laws. [Pg.240]

Based on Pascal s law, engineers can use two or more cylinders in a fluid power system. With the same pressure applied to both cylinders pictured in Figure 11-17, engineers can change the output force of each cylinder. How By changing the piston surface area of each cylinder. [Pg.244]

Pascal s law states that pressure in a container is equal throughout for both liquids and gases. [Pg.247]

Pascal s law Pascal s law states that when there is an increase in pressure at any point in a confined fluid, there is an equal increase at every other point in the container, passive solar heating Passive solar heating is solar energy absorbed by stone, slate, or other materials that radiates back into the air. patent A patent is a unique number assigned to an invention by the U.S. Patent Office that protects... [Pg.419]

Pascal, Blaise (1623-62) French mathematician and physicist. An infant prodigy, he had aheady made a mechanical calculating machine by 1642. in physics he formulated Pascal s law concerning fluid pressure and the principle behind the hydraulic press. The Si unit of pressure is named after him. [Pg.602]


See other pages where Pascal s law is mentioned: [Pg.585]    [Pg.587]    [Pg.592]    [Pg.631]    [Pg.46]    [Pg.794]    [Pg.173]    [Pg.767]    [Pg.19]    [Pg.661]    [Pg.160]    [Pg.246]    [Pg.239]    [Pg.245]    [Pg.247]   
See also in sourсe #XX -- [ Pg.4 ]

See also in sourсe #XX -- [ Pg.206 , Pg.220 ]

See also in sourсe #XX -- [ Pg.206 , Pg.220 ]

See also in sourсe #XX -- [ Pg.220 , Pg.221 , Pg.222 , Pg.228 ]

See also in sourсe #XX -- [ Pg.111 ]




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