/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 53 Consider a semicylindrical troug... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

Consider a semicylindrical trough of radius \(R\) and length \(L\) Develop general expressions for the magnitude and line of action of the hydrostatic force on one end, if the trough is partially filled with water and open to atmosphere. Plot the results (in nondimensional form) over the range of water depth \(0 \leq d / R \leq 1\).

Short Answer

Expert verified
The hydrostatic force exerted on one end of the trough is given by \( F = \gamma \cdot d \cdot \frac{1}{2} \pi R^{2} \), and it acts through the centroid of the end of the trough, which is at a depth of \( d - \frac{4R}{3\pi} \) from the water surface. The force increases linearly with the nondimensional water depth from 0 to 1.

Step by step solution

01

Define Variables

Let's denote the unit weight of water as \( \gamma \) and the depth of the water as \( d \). The semicylindrical trough has radius \( R \) and length \( L \).
02

Calculate Hydrostatic Force

The hydrostatic force exerted on the end of the trough can be calculated using the formula for the force exerted by a fluid on a surface, \( F = p \cdot A \), where \( p \) is the pressure and \( A \) is the area. Since the pressure due to a fluid column is given by \( p = \gamma \cdot d \), and the area of one end of the semicylindrical trough is \( A = \frac{1}{2} \pi R^{2} \), we find \( F = \gamma \cdot d \cdot \frac{1}{2} \pi R^{2} \).
03

Compute Line of Action

The line of action of the force is through the centroid of the area of the end of the trough, due to the symmetry of pressure distribution above and below the centroid of the semicircle. As we know, for a semicircle, the distance of the centroid from the base (line of diameter) is \( \frac{4R}{3\pi} \). The centroid is thus a depth of \( d - \frac{4R}{3\pi} \) from the water surface.
04

Dimensionless Depth and Its Variation

The nondimensional depth of water, given as \( d/R \), varies in the range 0 to 1. This means that we are considering all cases from the trough being empty (0) to the trough being completely full (1).
05

Plot the Results

Upon graphing the magnitude of the hydrostatic force against \( d/R \), we would find that the hydrostatic force linearly increases with \( d/R \), indicating that the force exerted by the water increases as the water depth increases. Note that this is a theoretical graph and real-world observations may vary due to factors like water turbulence.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Cast iron or steel molds are used in a horizontalspindle machine to make tubular castings such as liners and tubes. A charge of molten metal is poured into the spinning mold. The radial acceleration permits nearly uniformly thick wall sections to form. A steel liner, of length \(L=6 \mathrm{ft}\), outer radius \(r_{o}=6\) in. and inner radius \(r_{i}=4\) in., is to be formed by this process. To attain nearly uniform thickness, the angular velocity should be at least 300 rpm. Determine (a) the resulting radial acceleration on the inside surface of the liner and (b) the maximum and minimum pressures on the surface of the mold.

Assuming the bulk modulus is constant for seawater, derive an expression for the density variation with depth, \(h\) below the surface. Show that the result may be written \\[ \rho \approx \rho_{0}+b h \\] where \(\rho_{0}\) is the density at the surface. Evaluate the constant \(b .\) Then, using the approximation, obtain an equation for the variation of pressure with depth below the surface. Determine the depth in feet at which the error in pressure predicted by the approximate solution is 0.01 percent.

A partially full can of soda is placed at the outer edge of a child's merry- go-round, located \(R=5\) ft from the axis of rotation. The can diameter and height are 2.5 in. and 5 in. respectively. The can is half full, and the soda has specific gravity \(\mathrm{SG}=1.05 .\) Evaluate the slope of the liquid surface in the can if the merry-go-round spins at 20 rpm. Calculate the spin rate at which the can would spill, assuming no slippage between the can bottom and the merry-go-round. Would the can most likely spill or slide off the merry-go-round?

A proposed ocean salvage scheme involves pumping air into "bags" placed within and around a wrecked vessel on the sea bottom. Comment on the practicality of this plan, supporting your conclusions with analyses.

A canoe is represented by a right semicircular cylinder, with \(R=1.2 \mathrm{ft}\) and \(L=17 \mathrm{ft} .\) The canoe floats in water that is \(d=1 \mathrm{ft}\) deep. Set up a general algebraic expression for the total mass (canoe and contents) that can be floated, as a function of depth. Evaluate for the given conditions. Plot the results over the range of water depth \(0 \leq d \leq R\).

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.