What Is the Hydrostatic Force on a Vertical Gate in an Irrigation Canal?

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SUMMARY

The hydrostatic force on a trapezoidal gate in an irrigation canal, measuring 3 feet wide at the bottom and 5 feet wide at the top with a height of 2 feet, can be calculated using the formula for hydrostatic pressure. The density of water is taken as 60 lb/ft³. The force varies with depth, requiring integration of the pressure over the area of the gate. The total hydrostatic force is determined by evaluating the integral 60∫₀² y(5-y) dy, which accounts for the changing width of the gate at different depths.

PREREQUISITES
  • Understanding of hydrostatic pressure principles
  • Familiarity with integration techniques in calculus
  • Knowledge of trapezoidal geometry
  • Basic concepts of weight density versus mass density
NEXT STEPS
  • Study hydrostatic pressure calculations in fluid mechanics
  • Learn integration techniques for calculating areas under curves
  • Explore applications of hydrostatic force in engineering contexts
  • Investigate the properties of trapezoids and their applications in fluid dynamics
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Students and professionals in civil engineering, fluid mechanics, and physics who are involved in designing and analyzing hydraulic structures such as gates and dams.

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A gate in an irrigation canal is in the form of a trapezoid 3 feet wide at the bottom, 5 feet wide at the top, with the height equal to 2 feet. It is placed vertically in the canal with the water extending to its top. For simplicity, take the density of water to be 60 lb/ft cubed. Find the hydrostatic force in pounds on the gate.

I am having problems setting this problem up. It looks like its really easy but I am just not sure how to start it.

I know F = density x gravity x area x depth
 
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Because the force acts on the gate is not constant, i.e. force at the bottom is larger than that at the top , we have
dF = density x gravity x depth x d(area)
Do this integration over the trapezoid will yield the correct answer.
 
Imagine the gate being divided into many narrow horizontal bands of width "\Delta y". If y is the depth of a band, and \Delta y is small enough that we can think of every point in the band as at depth y, then the force along that band is the pressure, 60(y) [NOT "times gravity"! The density of the water is weight density, not mass density!], times the area: the length of the band times \Delta y. Of course, the length of the band depends on y: it is a linear function of y since the sides are straight lines, length(2)= 3 and length(0)= 5 so length(y)= -y+ 5. The force on that narrow band is 60y(5-y)\Delta y. The total force on the gate is the sum of those,\Sum 60y(5-1y)\Delta y, as y goes from 0 to 2. In the limit, that becomes the integral
60\int_0^5 y(5-y)dy
 

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