/*! 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 64 On the afternoon of January \(15... [FREE SOLUTION] | 91Ó°ÊÓ

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On the afternoon of January \(15,1919,\) an unusually warm day in Boston, a 17.7 -m-high, 27.4-m-diameter cylindrical metal tank used for storing molasses ruptured. Molasses flooded into the streets in a 5-m-deep stream, killing pedestrians and horses and knocking down buildings. The molasses had a density of \(1600 \mathrm{~kg} / \mathrm{m}^{3}\). If the tank was full before the accident, what was the total outward force the molasses exerted on its sides? (Hint: Consider the outward force on a circular ring of the tank wall of width \(d y\) and at a depth \(y\) below the surface. Integrate to find the total outward force. Assume that before the tank ruptured, the pressure at the surface of the molasses was equal to the air pressure outside the tank.)

Short Answer

Expert verified
The total outward force exerted by the molasses on the tank walls can be found by using the principles of fluid statics to find the pressure at a depth in the fluid and integrating this over the height of the tank. The result will be the force exerted by the molasses on the tank.

Step by step solution

01

Finding the Pressure at a Depth \(y\) in the Tank

The pressure at a depth \(y\) in a fluid of density \(\rho\) under the effect of gravity \(g\) is given by: \[P = P_{0} + \rho g y\] Here, \(P_{0}\) is the pressure at the surface of the fluid, which is given as equal to the air pressure. In our problem, \(\rho = 1600 \mathrm{~kg} / \mathrm{m}^{3}\), \(g = 9.8 \mathrm{~m/s}^{2}\) (standard value) and \(P_{0} = 1.01 \times 10^{5} \mathrm{~Pa}\) is the standard atmospheric pressure.
02

Computing the Differential Outward Force

Consider a small horizontal strip of the tank wall at depth \( y \) with a thickness \( dy \). The area of this strip is \( dA = 2 \pi r dy \), where \( r \) is the radius of the tank. Since the pressure acts perpendicular to a surface, the differential force on this strip is \( dF = P dA \). This can be substituted into the earlier pressure equation to get \[dF = g \rho r (2 \pi dy) y + P_{0} 2 \pi r dy\]
03

Integrating to find Total Outward Force

We must integrate this expression over the depth \( y \) from \( 0 \) to \( h \), where \( h \) is the height of the tank, to find the total outward force \( F \). \[ F = \int_{0}^{h} [g \rho r (2 \pi y) + P_{0} 2 \pi r] dy \] This can be split into two integrals and solved to find the total outward force.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Pressure Calculation
Understanding pressure calculation is crucial when dealing with fluid mechanics, an important part of physics. Pressure is defined as force exerted per unit area. In fluid pressure physics, this becomes particularly relevant when determining the force fluids apply on container walls or any submerged object.

To calculate the pressure at a certain depth within a fluid, like molasses in the given problem, we use the formula:
\[P = P_0 + \rho g y\]
Here, \(P\) represents the pressure at depth \(y\), \(P_0\) is the atmospheric pressure at the fluid's surface, \(\rho\) is the fluid's density, \(g\) is the acceleration due to gravity, and \(y\) is the depth within the fluid from the surface. This formula stems from the fact that fluid pressure increases with depth due to the weight of the fluid above pressing down.

To apply this to real-world problems, such as the catastrophic molasses storage tank rupture in Boston, it's imperative to understand that the pressure exerted by the fluid is not uniform. It increases with depth, leading to a greater force on the lower sections of the tank wall. By starting with the basic pressure calculation and considering the tank's dimensions and molasses density, one can begin to determine the total force acting on the tank's sides. This pressure calculation is foundational to analyzing the potential stress that led to the tank's failure.
Hydrostatics
Hydrostatics, a subfield of fluid mechanics, is the study of fluids at rest and the forces they exert. It's pertinent in understanding phenomena like the bursting of the Boston molasses tank. A foundational concept in hydrostatics is that the pressure at any point within a fluid at rest depends only on the depth at that point, not on the container's shape.

When dealing with liquids such as molasses, which are typically incompressible, hydrostatic principles allow us to reliably predict pressure increases with depth. The increase is linear if the fluid density is constant, as represented by the linear term in the pressure equation related to depth \(y\).

Moreover, hydrostatics helps explain why structures like tanks must be stronger at the base, where fluid pressure is highest. In practical engineering applications, like storage tanks design, the principles of hydrostatics guide architects and engineers in calculating wall thicknesses and materials needed to withstand the fluid pressures at different heights.
Integration in Physics
Integration is a mathematical tool widely used in various areas of physics to compute quantities that are spread out over a range of values. In the case of fluid pressure and force calculation on containers, integration allows us to sum up the forces acting over a continuous surface area.

In the context of the original problem involving the molasses tank, to find the total outward force on the tank's cylindrical wall, the differential force acting on an infinitesimally thin horizontal strip of the tank is first calculated. Each strip experiences a different pressure, which is a function of its depth in the fluid, and thus a different force. The integration process then involves adding up the force contributions from all these strips from the top to the bottom of the tank by integrating over the height of the tank:
\[ F = \int_0^h [g \rho r (2 \pi y) + P_0 2 \pi r] dy \]
Through integration, we get an exact value for the total outward force exerted by the fluid on the tank wall. This process is a powerful demonstration of how calculus, specifically integration, is vital in translating fundamental physics principles into quantitative predictions and solutions in real-world problems.

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