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Many altimeters determine altitude changes by measuring changes in the air pressure. An altimeter that is designed to be able to detect altitude changes of \(100 \mathrm{~m}\) near sea level should be able to detect pressure changes of a) approximately \(1 \mathrm{~Pa}\). d) approximately \(1 \mathrm{kPa}\). b) approximately 10 Pa. e) approximately \(10 \mathrm{kPa}\). c) approximately \(100 \mathrm{~Pa}\).

Short Answer

Expert verified
Answer: d) approximately 1 kPa

Step by step solution

01

Familiarize yourself with the Barometric Formula

The barometric formula is a mathematical model that relates atmospheric pressure to altitude. Near sea level, it is given by: $$ P(h) = P_{0}e^{\frac{-Mgh}{RT_{0}}}, $$ where \(P(h)\) is the atmospheric pressure at altitude \(h\), \(P_{0}\) is the atmospheric pressure at sea level, \(M\) is the molar mass of Earth's air, \(g\) is the acceleration due to gravity, \(R\) is the ideal gas constant, and \(T_{0}\) is the temperature at sea level.
02

Calculate the pressure at the initial altitude (0 m)

First, we need to find the atmospheric pressure at sea level (0 m). The given parameters are: - P0 = 101325 Pa - M = 0.029 kg/mol - g = 9.81 m/s^2 - R = 8.314 J/(mol*K) - T0 = 273.15 K (standard temperature at sea level) Using these values and the barometric formula, we get the pressure at sea level: $$ P(0) = 101325e^{\frac{-0.029*9.81*0}{8.314*273.15}} = 101325 \mathrm{~Pa}. $$
03

Calculate the pressure at the final altitude (100 m)

Now, we need to find the atmospheric pressure at an altitude of 100 m. Using the given parameters and the barometric formula, we get the pressure at 100 m: $$ P(100) = 101325e^{\frac{-0.029*9.81*100}{8.314*273.15}} \approx 100246.2 \mathrm{~Pa}. $$
04

Determine the pressure change

To find the pressure change that the altimeter should be able to detect, subtract the pressure at the initial altitude (0 m) from the final altitude (100 m): $$ \Delta P = P(100) - P(0) \approx 100246.2 - 101325 \approx -1078.8 \mathrm{~Pa}. $$ Since we are only interested in the magnitude of the pressure change, we can take the absolute value: $$ |\Delta P| \approx 1078.8 \mathrm{~Pa}. $$
05

Compare the calculated pressure change to the given options

From the calculated pressure change, we can see that the closest option to the correct value is d) approximately 1 kPa. Note that 1 kPa = 1000 Pa, which is close to the calculated value of 1078.8 Pa. So, the correct answer is option d).

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Key Concepts

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

Understanding Atmospheric Pressure
Atmospheric pressure is the force exerted by the weight of the air above us and is a fundamental concept in understanding weather, climate, and how altimeters work. It's measured in pascals (Pa) and typically decreases as altitude increases due to the thinning of the air. This is precisely why altimeters, which are instruments used to measure altitude, are based on the detection of these pressure changes. Simplifying this, imagine the atmosphere as a stack of air layers; the higher you go, the fewer layers press down on you, resulting in lower pressure.

For practical applications like aviation, knowing the atmospheric pressure is crucial for pilots to determine their elevation above sea level. Altimeters aid in this process by responding to the pressure changes, allowing pilots to navigate safely by maintaining the correct altitude. It's a fine balance, as the difference between safe flying and potential danger could just be a matter of a few hundred pascals.
The Impact of Altitude Changes
Altitude changes are directly related to changes in atmospheric pressure, and understanding this relationship is essential for various activities ranging from aviation to meteorology. As mentioned earlier, air pressure decreases with an increase in altitude. But why does this matter? For one, hikers and climbers often experience the effects of altitude in the form of 'thin air,' which can make breathing more laborious.

Moreover, the barometric formula shows us that these pressure changes are exponential, not linear. This means that the rate at which pressure decreases is not the same at all altitudes; it's faster at lower altitudes and slower at higher ones. As a result, an altimeter designed to detect changes at sea level needs to be sensitive to relatively small changes in air pressure, as the exercise illustrates.
Interpreting the Ideal Gas Law in Context
The ideal gas law, represented by the equation PV=nRT (where P is pressure, V is volume, n is the number of moles, R is the universal gas constant, and T is temperature), provides the theoretical foundation to understand how gases behave under different conditions of temperature, pressure, and volume. In the context of atmospheric pressure and altitude, the barometric formula can be seen as an application of the ideal gas law tailored to the Earth’s atmosphere.

Diving deeper into the exercise, we see how the ideal gas law is implicitly used to derive the barometric formula for atmospheric pressure at different altitudes. The values for the molar mass of air (M), the gravity (g), and the ideal gas constant (R) work together with the standard temperature at sea level (T0) to predict how pressure decreases with altitude. The barometric formula is a reminder that the air above us behaves according to universal gas laws, and by measuring its pressure, we unlock information about altitude and much more.

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Most popular questions from this chapter

A fountain sends water to a height of \(100 . \mathrm{m}\). What is the difference between the pressure of the water just before it is released upward and the atmospheric pressure?

You are in a boat filled with large rocks in the middle of a small pond. You begin to drop the rocks into the water. What happens to the water level of the pond? a) It rises. d) It rises momentarily and then b) It falls. falls when the rocks hit bottom. c) It doesn't change. e) There is not enough information to say.

Water of density \(998.2 \mathrm{~kg} / \mathrm{m}^{3}\) is moving at negligible speed under a pressure of \(101.3 \mathrm{kPa}\) but is then accelerated to high speed by the blades of a spinning propeller. The vapor pressure of the water at the initial temperature of \(20.0^{\circ} \mathrm{C}\) is \(2.3388 \mathrm{kPa}\). At what flow speed will the water begin to boil? This effect, known as cavitation, limits the performance of propellers in water

You fill a tall glass with ice and then add water to the level of the glass's rim, so some fraction of the ice floats above the rim. When the ice melts, what happens to the water level? (Neglect evaporation, and assume that the ice and water remain at \(0^{\circ} \mathrm{C}\) during the melting process.) a) The water overflows the rim. b) The water level drops below the rim. c) The water level stays at the top of the rim. d) It depends on the difference in density between water and ice.

The atmosphere of Mars exerts a pressure of only 600\. Pa on the surface and has a density of only \(0.0200 \mathrm{~kg} / \mathrm{m}^{3}\). a) What is the thickness of the Martian atmosphere, assuming the boundary between atmosphere and outer space to be the point where atmospheric pressure drops to \(0.0100 \%\) of its yalue at surface level? b) What is the atmospheric pressure at the bottom of Mars's Hellas Planitia canyon, at a depth of \(7.00 \mathrm{~km} ?\) c) What is the atmospheric pressure at the top of Mars's Olympus Mons volcano, at a height of \(27.0 \mathrm{~km} ?\) d) Compare the relative change in air pressure, \(\Delta p / p\), between these two points on Mars and between the equivalent extremes on Earth-the Dead Sea shore, at \(400 . \mathrm{m}\) below sea level, and Mount Everest, at an altitude of \(8850 \mathrm{~m}\).

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