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What is the atmospheric pressure on top of Mt. Everest on a day when water boils there at a temperature of \(70.0^{\circ} \mathrm{C} ?\)

Short Answer

Expert verified
The atmospheric pressure on top of Mt. Everest on a day when water boils at 70.0°C is approximately 233 mb (millibars) or hPa (hectopascals).

Step by step solution

01

Understand the Relationship Between Boiling Point and Atmospheric Pressure

The boiling point of a liquid varies according to the atmospheric pressure. At standard atmospheric pressure (1 atm), pure water boils at a temperature of 100 degrees Celsius. At higher altitudes, the atmospheric pressure is lower, and therefore water boils at a lower temperature. To find the atmospheric pressure at the top of Mt. Everest, one can use the fact that water is boiling at 70.0°C to estimate the atmospheric pressure.
02

Use the Clausius-Clapeyron Relation

The Clausius-Clapeyron equation can be used to estimate the vapor pressure at a certain temperature. However, tables or an equation of state that describes the relationship between the boiling point of water and the pressure may be more convenient and practical to use since the calculation can be complex.
03

Consult a Water Boiling Point at Different Pressures Table or Calculator

By consulting a table or a calculator that shows the boiling point of water at various pressures, one can determine the atmospheric pressure corresponding to the known boiling point of 70.0°C. Such tables are derived from experimental data and provide a straightforward way to find the pressure without complex calculations.
04

Determine the Pressure

From standard tables, one can find that the boiling point of water is 70.0°C at an atmospheric pressure of approximately 233 millibars (mb) or hectopascals (hPa). Therefore, this is the pressure at the top of Mt. Everest on a day when water boils there at 70.0°C.

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Key Concepts

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

Boiling Point and Atmospheric Pressure
When we talk about the boiling point of water, many immediately think of the standard 100°C, but this temperature isn't a constant—it varies with atmospheric pressure. For instance, at sea level, the atmospheric pressure is about 1 atm, and water boils at 100°C. However, if you climb to a place like Mt. Everest, the pressure drops, and so does the boiling point of water.

At high altitudes where the atmosphere is thinner, there's less air pushing down on the water's surface. Because of this reduced external pressure, it takes less energy for the water molecules to escape into the air; hence, water boils at a lower temperature. This relationship is profound because it demonstrates the interconnectivity between physical properties and environmental conditions. In cooking and industrial processes, this knowledge is crucial to adjust for the changes in boiling temperature due to pressure variations.
Clausius-Clapeyron Equation
The Clausius-Clapeyron equation is a fancy name for a simple concept with profound implications: it describes how the pressure of a liquid's vapor changes as the temperature changes. Mathematically, this is represented as \( \frac{dP}{dT} = \frac{L}{T \Delta V} \), where \( \frac{dP}{dT} \) is the rate of change in pressure with temperature, \( L \) is the latent heat of vaporization, \( T \) is the temperature in Kelvin, and \( \Delta V \) is the change in volume.

It is a powerful tool in thermodynamics but can be complex to apply directly. However, the equation is foundational for tables and calculators that relate boiling points to pressure, allowing us to bypass intricate calculations and obtain practical estimates quickly.
Vapor Pressure Estimation
Understanding vapor pressure is vital in many fields, from meteorology to the culinary arts. Vapor pressure is essentially the pressure exerted by a vapor in equilibrium with its liquid or solid form. It is a specific indication of a liquid's evaporation rate at a given temperature. The ability to estimate this pressure comes in handy, particularly when you need to determine boiling points under varying atmospheric conditions.

To estimate vapor pressure without heavy-duty calculations, one can employ the aforementioned Clausius-Clapeyron equation or rely on simpler empirical formulas. A common method also includes using established reference tables that give us the boiling points of various substances at different pressures, freeing us from the mental gymnastics of the more complex physics.
Water Boiling Point Table
Boiling point tables are like cheat sheets for quick reference when we need to know at what temperature water (or any liquid) will boil under a specific pressure. These tables are plotted from experimental data and are incredibly user-friendly, offering a direct correlation between pressure (often in atmospheres, millibars, or mmHg) and the boiling temperature.

For example, if you're on top of Mt. Everest, and if you know that water boils at about 70°C, you can simply look at the table and find the corresponding atmospheric pressure, sidestepping the need for complex formulae and calculations. These tables serve as an essential tool for a variety of applications, ranging from culinary preparation adjustments in high-altitude cities to scientific experiments where controlling temperature and pressure is critical.

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Most popular questions from this chapter

A researcher measures the wavelength of a 1.20-GHz electromagnetic wave to be \(0.500 \mathrm{~m}\). (a) Calculate the speed at which (b) What is unreasonable about this result? this wave propagates. (c) Which assumptions are unreasonable or inconsistent?

The vapor pressure of water at \(40.0^{\circ} \mathrm{C}\) is \(7.34 \times 10^{3} \mathrm{N} / \mathrm{m}^{2} .\) Using the ideal gas law, calculate the density of water vapor in \(\mathrm{g} / \mathrm{m}^{3}\) that creates a partial pressure equal to this vapor pressure. The result should be the same as the saturation vapor density at that temperature \(\left(51.1 \mathrm{g} / \mathrm{m}^{3}\right)\).

(a) Suppose a cold front blows into your locale and drops the temperature by 40.0 Fahrenheit degrees. How many degrees Celsius does the temperature decrease when there is a \(40.0^{\circ} \mathrm{F}\) decrease in temperature? (b) Show that any change in temperature in Fahrenheit degrees is nine-fifths the change in Celsius degrees.

Air in human lungs has a temperature of \(37.0^{\circ} \mathrm{C}\) and a saturation vapor density of \(44.0 \mathrm{g} / \mathrm{m}^{3}\). (a) If \(2.00 \mathrm{L}\) of air is exhaled and very dry air inhaled, what is the maximum loss of water vapor by the person? (b) Calculate the partial pressure of water vapor having this density, and compare it with the vapor pressure of \(6.31 \times 10^{3} \mathrm{N} / \mathrm{m}^{2}\).

What is the maximum electric field strength in an electromagnetic wave that has a maximum magnetic field strength of \(5.00 \times 10^{-4} \mathrm{~T}\) (about 10 times the Earth's)?

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