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  1. Dec 28, 2020 · Pressure is a key concept in physics, whether you're interested in how meteorologists predict the weather, or you want to describe the Carnot cycle in thermodynamics. Pressure is the force on a surface per unit area, and it has a close link to the temperature of the liquid or gas creating it.

  2. The pressure gauge on her air tank reads \(6.9 \times 10^6 \, Pa\). What force does the air inside the tank exert on the flat end of the cylindrical tank, a disk 0.150 m in diameter? Strategy. We can find the force exerted from the definition of pressure (Equation \red{pressure}) provided we can find the area \(A\) acted upon. Solution

  3. Pressure. Pressure (p) is defined as the normal force F per unit area A over which the force is applied, or \[p = \frac{F}{A} \ldotp \label{14.3}\] To define the pressure at a specific point, the pressure is defined as the force dF exerted by a fluid over an infinitesimal element of area dA containing the point, resulting in p = \(\frac{dF}{dA}\).

  4. Jun 1, 2021 · The units of pressure depend on the units of area: If the area is measured in cm 2 (and the force in N), then the pressure will be in N/cm 2; If the area is measured in m 2 (and the force in N), then the pressure will be in N/m 2; Pressure can also be measured in pascals, Pa where 1 Pa is the same as 1 N/m 2; Pressure, unlike force, is a scalar.

  5. Fluid pressure has no direction, being a scalar quantity. The forces due to pressure have well-defined directions: they are always exerted perpendicular to any surface. (See the tire in , for example.) Finally, note that pressure is exerted on all surfaces. Swimmers, as well as the tire, feel pressure on all sides. (See .)

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  7. We can find the force exerted from the definition of pressure given in [latex]P=\frac{F}{A}\\[/latex], provided we can find the area A acted upon. Solution. By rearranging the definition of pressure to solve for force, we see that. F = PA. Here, the pressure P is given, as is the area of the end of the cylinder A, given by A = π r 2. Thus,

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