Respuesta :

Answer:

[tex]\rho \cdot g[/tex], where [tex]\rho[/tex] is the density of the liquid, and [tex]g[/tex] is the value of gravitational acceleration.

Step-by-step explanation:

Let [tex]\rho[/tex] be the density of a liquid. Let [tex]g[/tex] represent the gravitational acceleration (near the surface of the earth, [tex]g \approx 9.81\; \rm N \cdot kg^{-1}[/tex].)

The pressure [tex]P[/tex] at a depth of [tex]h[/tex] under the surface of this liquid would be

[tex]P = \rho \cdot g \cdot h[/tex].

Here's how to deduce this equation from the definition of pressure.

Pressure is the amount of force on a surface per unit area. For example, if a force of [tex]1\; \rm N[/tex] is applied over a surface with an area of [tex]1\; \rm m^2[/tex], then the pressure on that surface would be [tex]\rm 1\; \rm Pa[/tex] (one Pascal.)

Consider a flat, square object that is horizontally submerged under some liquid at a depth of [tex]h[/tex]. Assume that [tex]A[/tex] is the area of that square. The volume of the liquid that sits on top of this square would be [tex]V = A \cdot h[/tex]. If the density of that liquid is [tex]\rho[/tex], then the mass of that much liquid would be [tex]m= \rho \cdot V= \rho \cdot A \cdot h[/tex].

The weight of that much liquid would be [tex]W = m \cdot g = \rho \cdot A \cdot h \cdot g[/tex]. The liquid on top of that object would exert a force of that size on the object. Since that force is exerted over an area of [tex]A[/tex], the pressure on the object would be

[tex]\displaystyle P = \frac{F}{A} = \frac{\rho \cdot A \cdot h \cdot g}{A} = \rho \cdot h \cdot g[/tex].

In this question, [tex]h = 1\; \rm m[/tex]. As a side note, if [tex]\rho[/tex] and [tex]g[/tex] are also in standard units ([tex]\rm kg \cdot m^{-3}[/tex] for [tex]\rho[/tex] and [tex]\rm N \cdot kg^{-1}[/tex] for [tex]g[/tex]), then [tex]P[/tex] would be in Pascals ([tex]\rm Pa[/tex], where [tex]1\; \rm Pa = 1\; \rm N \cdot m^{-2}[/tex].)

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