Pressures Exerted by Static Fluids

Overview of Fluid Mechanics Study

  • Focus: Physics of fluids, particularly pressure and force related to fluids in containers.

  • Course Segment: Completion of one-third of the course focusing on fluidity study.

Importance of Fluid Mechanics

  • Context: Fluid dynamics is crucial for industries handling large quantities of liquids, such as petroleum.

  • Objective: Determine how the weight of liquids affects the surfaces they contact and understand the forces involved.

    • Key Concept: Fluids exert pressure in all directions and do not have parallel forces; pressure is exerted uniformly in all directions.

Key Concepts and Equations

  • Fundamental Principle: The pressure exerted by fluids at any point can be calculated.

    • Pressure Equation: p=mAp = \frac{m}{A}

    • Where:

      • mm = mass,

      • AA = area over which the force is distributed.

    • General Format: Force is the cumulative pressure applied over a surface area (dAdA).

  • Pressure at a Fluid Depth:

    • Formula: p=ρghp = \rho g h

    • Where:

      • ρ\rho = density of the fluid,

      • gg = acceleration due to gravity,

      • hh = height of fluid column above the point.

Container Example

  • Container Setup: Analyze a container filled with liquid to understand forces at the bottom.

    • Pressure at the Bottom of Container (h):

    • Resultant pressure: Pressure=ρgh\text{Pressure} = \rho g h

    • Force Calculation:

      • Force at the bottom: F=p⋅dAF = p \cdot dA

      • dAdA defined as width times height dimensions.

    • Total Volume of Fluid:

    • Given by V=l×w×hV = l \times w \times h

  • Fluid Forces: Calculating horizontal/lateral forces as a function of fluid height (yy):

    • Lateral force increases with depth: force function integrates pressure throughout the depth of the fluid.

Integral Calculations

  • Integral of Horizontal Forces:

    • Force as a function of height can be integrated:

    • F=∫0hp⋅dAF = \int_0^h p \cdot dA

  • For Variable Height:

    • p(y)=ρgyp(y) = \rho g y

    • dA=wimesdydA = w imes dy

    • Therefore force becomes F=∫0hρgy⋅w dyF = \int_0^h \rho g y \cdot w \, dy

    • Result: F=ρgw∫0hy dy=ρgw⋅h22F = \rho g w \int_0^h y \, dy = \rho g w \cdot \frac{h^2}{2}

  • Average Location of Force:

    • To find the location of the resultant force, calculate the first moment of area:

    • Moment M1=∫y⋅dAM_1 = \int y \cdot dA yields the center of pressure location.

Resultant Forces and Location

  • Resultant Force Calculation:

    • Resultant horizontal force becomes FR=ρgw⋅h22F_R = \rho g w \cdot \frac{h^2}{2}

  • Location of the Force:

    • The average height for reinforcement based on pressure distribution: located at two-thirds of the fluid height, yR=23hy_R = \frac{2}{3}h

    • Reinforcement position becomes critical at 67% of the full height, which ensures adequate support against fluid pressure.

Considerations for Gates in Fluid Containers

  • Gate Placement Analysis:

    • When considering a gate within the fluid, re-evaluate forces from the fluid level (h<em>0h<em>0) to the height above the gate (h</em>1h</em>1).

  • Integration Limits for Gate Analysis:

    1. Begin at height h<em>0h<em>0 and end at h</em>0+h1h</em>0 + h_1.

    2. Apply the same pressure function integrated across the gate's height.

  • Resultant Force at the Gate:

    • Magnitude and location determined similarly, ensuring structural integrity for various fluid heights.

  • Special Cases in Design:

    • If h0=0h_0 = 0, pressures apply uniformly across the gate area and resultant modifications consider fluid density.

    • If h1=0h_1 = 0, the system has no force acting through the gate—critical for mechanical reinforcement designs.