/*! 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 34 At a height of \(10 \mathrm{~km}... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

At a height of \(10 \mathrm{~km}\) (33 \(000 \mathrm{ft}\) ) above sea level, atmospheric pressure is about \(210 \mathrm{~mm}\) of mercury. What is the net resultant normal force on a \(600 \mathrm{~cm}^{2}\) window of an airplane flying at this height? Assume the pressure inside the plane is \(760 \mathrm{~mm}\) of mercury. The density of mercury is \(13600 \mathrm{~kg}\).

Short Answer

Expert verified
The net resultant normal force on the window is 4401.56 N.

Step by step solution

01

Convert Atmospheric Pressure to Pascal

We start by converting the atmospheric pressure at a height of 10 km, which is given as 210 mm of mercury, into Pascal. Use the relation:\[ P = h \times \rho \times g \]where \(h = 210 \, \text{mm} = 0.21 \, \text{m}\), \(\rho = 13600 \, \text{kg/m}^3\) (density of mercury), and \(g = 9.81 \, \text{m/s}^2\) (acceleration due to gravity). Thus,\[ P_{\text{outside}} = 0.21 \times 13600 \times 9.81 = 27932.88 \, \text{Pa}\]
02

Convert Cabin Pressure to Pascal

Next, convert the pressure inside the airplane from 760 mm of mercury to Pascal using the same conversion method:\[ P_{\text{inside}} = h \times \rho \times g \]where \(h = 760 \, \text{mm} = 0.76 \, \text{m}\), \(\rho = 13600 \, \text{kg/m}^3\), and \(g = 9.81 \, \text{m/s}^2\). Thus,\[ P_{\text{inside}} = 0.76 \times 13600 \times 9.81 = 101292.16 \, \text{Pa}\]
03

Calculate Pressure Difference

Calculate the difference between the cabin pressure and the outside atmospheric pressure:\[ \Delta P = P_{\text{inside}} - P_{\text{outside}} \]Substitute the values:\[ \Delta P = 101292.16 - 27932.88 = 73359.28 \, \text{Pa} \]
04

Calculate the Resultant Normal Force

Now, calculate the net resultant normal force on the window using the pressure difference and the area of the window. The formula to compute force is:\[ F = \Delta P \times A \]where \(A = 600 \times 10^{-4} \, \text{m}^2 = 0.06 \, \text{m}^2\). Hence,\[ F = 73359.28 \times 0.06 = 4401.56 \, \text{N} \]

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!

Key Concepts

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

Pressure Conversion
Pressure conversion is a key concept when solving physics problems involving fluids and gases. Understanding how to convert pressure from one unit to another is essential for accurate calculations. In this exercise, we are dealing with atmospheric pressure measured in millimeters of mercury (mm Hg), which is a common unit in meteorology and aviation.

To convert pressure from mm Hg to Pascals (Pa), use the formula:
  • \(P = h \times \rho \times g\)
where:
  • \(h\) is the height of the mercury column (converted to meters)
  • \(\rho\) is the density of mercury, typically \(13600 \, \text{kg/m}^3\)
  • \(g\) is the acceleration due to gravity, approximately \(9.81 \, \text{m/s}^2\)
By substituting these values, you convert mm Hg to Pa to find the pressure exerted by the gas. This conversion is crucial to make our calculations compliant with the International System of Units (SI) and ensure the results are universally understandable. By doing this, the given atmospheric pressure of \(210 \, \text{mm Hg}\) was converted to \(27932.88 \, \text{Pa}\). This step allows for subsequent force calculations in the problem-solving process.
Normal Force Calculation
Calculating the normal force involves understanding the difference in pressure on two sides of a surface and how this differential translates into a force. In atmospheric physics, this is especially relevant, such as when examining the forces acting on airplane windows while flying at high altitudes.

The formula used to calculate the net resultant normal force is:
  • \(F = \Delta P \times A\)
where:
  • \(\Delta P\) represents the pressure difference across the surface (in Pascals)
  • \(A\) is the area of the surface (in square meters)
This method involves several steps:
  • First, find the pressure inside the cabin and outside using pressure conversion as shown earlier.
  • Then, calculate the pressure difference \(\Delta P\) by subtracting the external pressure from the internal pressure.
  • Finally, multiply this pressure difference by the surface area to find the force in newtons (N). In this problem, we calculated a normal force of \(4401.56 \, \text{N}\) on the airplane window, demonstrating the immense pressure differences managed by aircraft at high altitudes.
Atmospheric Physics
Atmospheric physics deals with understanding the physical processes and phenomena that occur in the atmosphere of Earth. This includes the study of pressure, temperature, and other atmospheric conditions that affect everything from weather patterns to commercial aviation.

A crucial aspect is understanding how atmospheric pressure changes with altitude. At sea level, atmospheric pressure is about \(1013.25 \, \text{hPa}\) or \(760 \, \text{mm Hg}\). However, as altitude increases, the pressure decreases because there's less air above to exert a force downward. This is seen in our exercise where at \(10 \, \text{km}\) above sea level, the atmospheric pressure drops to \(210 \, \text{mm Hg}\).

This decrease in pressure affects various aspects of aviation, including the structural integrity of an airplane. Engineers must precisely calculate pressures and forces to ensure safe and efficient aircraft design. This involves understanding not just the static pressures but also dynamic changes during flight conditions. Basic concepts of atmospheric physics thus play a vital role in engineering and design considerations in aerospace and other fields related to the atmosphere.

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

A 2.0-cm cube of metal is suspended by a fine thread attached to a scale. The cube appears to have a mass of \(47.3 \mathrm{~g}\) when measured submerged in water. What will its mass appear to be when submerged in glycerin, sp gr = 1.26? [Hint: Find \(\rho\) too.]

The U-tube device connected to the tank in Fig. 13-6 is called a manometer. As you can see, the mercury in the tube stands higher in one side than the other. What is the pressure in the tank if atmospheric pressure is \(76 \mathrm{~cm}\) of mercury? The density of mercury is \(13.6 \mathrm{~g} / \mathrm{cm}^{3}\). from which \(P=95 \mathrm{kPa}\). Or, more simply perhaps, we could note that the pressure in the tank is \(5.0 \mathrm{~cm}\) of mercury lower than atmospheric. So the pressure is \(71 \mathrm{~cm}\) of mercury, which is \(94.6 \mathrm{kPa}\).

A partly filled beaker of water sits on a scale, and its weight is \(2.30 \mathrm{~N}\). When a piece of metal suspended from a thread is totally immersed in the beaker (but not touching bottom), the scale reads \(2.75 \mathrm{~N}\). What is the volume of the metal? The water exerts an upward buoyant force on the metal. According to Newton's Third Law of action and reaction, the metal exerts an equal downward force on the water. It is this force that increases the scale reading from \(2.30 \mathrm{~N}\) to \(2.75 \mathrm{~N}\). Hence the buoyant force is \(2.75-2.30=0.45 \mathrm{~N}\). Then, because \(F_{B}=\) weight of displaced water \(=\rho_{w} g V=\left(1000 \mathrm{~kg} / \mathrm{m}^{3}\right)\left(9.81 \mathrm{~m} / \mathrm{s}^{2}\right)(V)\) we have the volume of the displaced water, and of the piece of metal, namely, $$ V=\frac{0.45 \mathrm{~N}}{9810 \mathrm{~kg} / \mathrm{m}^{2} \cdot \mathrm{s}^{2}}=46 \times 10^{-6} \mathrm{~m}^{3}=46 \mathrm{~cm}^{3} $$

When a submarine dives to a depth of \(120 \mathrm{~m}\), to how large a total pressure is its exterior surface subjected? The density of seawater is about \(1.03 \mathrm{~g} / \mathrm{cm}^{3}\) \(P=\) Atmospheric pressure \(+\) Pressure of wate $$ \begin{array}{l} =1.01 \times 10^{5} \mathrm{~N} / \mathrm{m}^{2}+\rho g h=1.01 \times 10^{5} \mathrm{~N} / \mathrm{m}^{2}+\left(1030 \mathrm{~kg} / \mathrm{m}^{3}\right)\left(9.81 \mathrm{~m} / \mathrm{s}^{2}\right)(120 \mathrm{~m}) \\ =1.01 \times 10^{5} \mathrm{~N} / \mathrm{m}^{2}+12.1 \times 10^{5} \mathrm{~N} / \mathrm{m}^{2}=13.1 \times 10^{5} \mathrm{~N} / \mathrm{m}^{2}=1.31 \mathrm{MPa} \end{array} $$

A wooden cylinder has a mass \(m\) and a base area \(A\). It floats in water with its axis vertical. Show that the cylinder undergoes SHM if given a small vertical displacement. Find the frequency of its motion. When the cylinder is pushed down a distance \(y\), it displaces an additional volume Ay of water. Because this additional displaced volume has mass \(A y_{\rho w}\), an additional buoyant force \(A y_{\rho w g}\) acts on the cylinder, where \(\rho_{w}\) is the density of water. This is an unbalanced force on the cylinder and is a restoring force. In addition, the force is proportional to the displacement and so is a Hooke's Law force. Therefore, the cylinder will undergo SHM, as described in Chapter 11 . Comparing \(F_{B}=A \rho_{w} g y\) with Hooke's Law in the form \(F=k y\), we see that the elastic constant for the motion is \(k=A \rho_{w} g .\) This, acting on the cylinder of mass \(m\), causes it to have a vibrational frequency of $$ f=\frac{1}{2 \pi} \sqrt{\frac{k}{m}}=\frac{1}{2 \pi} \sqrt{\frac{A \rho_{w} g}{m}} $$

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.