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Titan, the largest satellite of Saturn, has a thick nitrogen atmosphere. At its surface, the pressure is 1.5 earth-atmospheres and the temperature is 94 K. (a) What is the surface temperature in \(^\circ\)C? (b) Calculate the surface density in Titan's atmosphere in molecules per cubic meter. (c) Compare the density of Titan's surface atmosphere to the density of earth's atmosphere at 22\(^\circ\)C. Which body has denser atmosphere?

Short Answer

Expert verified
(a) -179.15°C; (b) 2.68x10^25 molecules/m^3; (c) Titan's atmosphere is denser.

Step by step solution

01

Convert to Celsius

To find the temperature in Celsius for part (a), use the formula for conversion between Kelvin and Celsius: \[T(\text{°C}) = T(\text{K}) - 273.15\]Given, \(T(\text{K}) = 94\) K, so:\[T(\text{°C}) = 94 - 273.15 = -179.15\, \text{°C}\]
02

Use Ideal Gas Law for Surface Density

For part (b), we use the ideal gas law to find the density \(\rho\) (mass per volume) in molecules per cubic meter. The ideal gas law in terms of density is:\[P = \rho \cdot \frac{k_B \cdot T}{m}\]where \( P \) is pressure, \( \rho \) is density, \( k_B \) is Boltzmann's constant \(1.38 \times 10^{-23} \text{ J/K} \), \( T \) is temperature, and \( m \) is the mass of one molecule of nitrogen \(4.65 \times 10^{-26} \text{ kg}\).Given \( P = 1.5\) atm, we first convert it to Pa:\(P = 1.5 \times 1.013 \times 10^5 = 1.5195 \times 10^5 \text{ Pa}\).The density expression becomes:\[\rho = \frac{P \cdot m}{k_B \cdot T} = \frac{1.5195 \times 10^5 \times 4.65 \times 10^{-26}}{1.38 \times 10^{-23} \times 94}= 2.68 \times 10^{25} \text{ molecules/m}^3\]
03

Compare with Earth's Atmospheric Density

For part (c), we need Earth's atmospheric density at \(22\,°\text{C} = 295\,\text{K}\). Using the ideal gas law, the density on Earth \(\rho_{\text{Earth}}\) can be similarly calculated (assuming nitrogen dominates Earth's atmosphere too) with atmospheric pressure \(1.013 \times 10^5 \text{ Pa}\):\[\rho_{\text{Earth}} = \frac{1.013 \times 10^5 \times 4.65 \times 10^{-26}}{1.38 \times 10^{-23} \times 295}= 2.42 \times 10^{25} \text{ molecules/m}^3\]Thus, Titan's surface atmosphere is denser than Earth's at \(22\,°\text{C}\).
04

Conclusion: Compare Densities

Titan's atmospheric density \(2.68 \times 10^{25} \text{ molecules/m}^3\) is greater than Earth's atmospheric density \(2.42 \times 10^{25} \text{ molecules/m}^3\). Therefore, Titan has a denser atmosphere at its surface than Earth does at \(22\)°C.

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Key Concepts

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

Titan's Atmosphere
Titan, Saturn's largest moon, is a fascinating celestial body with a thick and dense atmosphere primarily composed of nitrogen, much like Earth's. This dense atmosphere makes Titan one of the most Earth-like bodies in our solar system in terms of atmospheric pressure and composition. However, it differs significantly in terms of temperature and surface conditions.
The atmosphere of Titan exerts a surface pressure that is about 1.5 times that of Earth's at sea level. This substantial pressure is intriguing considering Titan's position far out in the solar system, where one would typically expect much lower pressures and densities. The thick atmosphere also plays a crucial role in shaping Titan's landscape and weather, contributing to the presence of methane lakes and rivers on its surface.
Atmospheric Pressure Conversion
The conversion of pressure units is essential in understanding atmospheric conditions on different celestial bodies. In the case of Titan, the surface pressure is given as 1.5 Earth-atmospheres, where 1 atmosphere (atm) is equivalent to 101,325 Pascals (Pa). To convert Titan’s atmospheric pressure into Pascals, simply multiply by this conversion factor:
  • Pressure in Pascals: 1.5 atm = 1.5 × 101,325 Pa = 151,987.5 Pa or approximately 1.52 × 10^5 Pa.
Understanding this conversion is pivotal for applying the ideal gas law, which uses pressure in the SI unit of Pascals. This law helps us determine various properties of gases such as density and temperature, which are crucial for comparing atmospheric conditions between different planets or moons.
Temperature Conversion Kelvin to Celsius
Conversion from Kelvin to Celsius is a straightforward process that is essential for interpreting temperatures in a manner more familiar to everyday experiences. The formula for this conversion is \(T(\text{°C}) = T(\text{K}) - 273.15\), which allows us to convert temperatures from the Kelvin scale, often used in scientific calculations, to the Celsius scale.
For example, Titan's surface temperature is given as 94 Kelvin. Using the conversion formula:
  • \(T(\text{°C}) = 94 - 273.15 = -179.15\, \text{°C}\).
This conversion shows us how incredibly cold Titan's surface is compared to Earth, giving us insight into the harsh conditions that any probe or surface exploration technology would face.
Density Comparison
Density comparison is key in understanding the relative mass and distribution of atmospheric particles in different environments, which influences both weather phenomena and potential habitability. In this case, the ideal gas law helps us calculate and compare the atmospheric density on Titan to that on Earth.
Using the formula \(\rho = \frac{P \cdot m}{k_B \cdot T}\) from the ideal gas law:
  • The density of Titan's atmosphere was found to be about \(2.68 \times 10^{25} \text{ molecules/m}^3\).
Similarly, Earth's atmospheric density at 22°C (295 K) is approximately \(2.42 \times 10^{25} \text{ molecules/m}^3\). Despite temperatures and compositions being different, Titan's atmosphere is denser than Earth's. This difference highlights how Titan’s atmosphere is exceptionally thick for a moon far from the Sun, underscoring the unique conditions present on this intriguing satellite.

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Most popular questions from this chapter

Modern vacuum pumps make it easy to attain pressures of the order of 10\({^-}{^1}{^3}\) atm in the laboratory. Consider a volume of air and treat the air as an ideal gas. (a) At a pressure of 9.00\(\times\) 10\({^-}{^1}{^4}\) atm and an ordinary temperature of 300.0 K, how many molecules are present in a volume of 1.00 cm\(^3\)? (b) How many molecules would be present at the same temperature but at 1.00 atm instead?

Helium gas is in a cylinder that has rigid walls. If the pressure of the gas is 2.00 atm, then the root-mean-square speed of the helium atoms is \(\upsilon {_r}{_m}{_s}\) = 176 m/s. By how much (in atmospheres) must the pressure be increased to increase the \(\upsilon {_r}{_m}{_s}\) of the He atoms by 100 m/s? Ignore any change in the volume of the cylinder.

(a) Calculate the specific heat at constant volume of water vapor, assuming the nonlinear triatomic molecule has three translational and three rotational degrees of freedom and that vibrational motion does not contribute. The molar mass of water is 18.0 g/mol. (b) The actual specific heat of water vapor at low pressures is about 2000 J/kg \(\cdot\) K. Compare this with your calculation and comment on the actual role of vibrational motion.

A cylinder 1.00 m tall with inside diameter 0.120 m is used to hold propane gas (molar mass 44.1 g/mol) for use in a barbecue. It is initially filled with gas until the gauge pressure is 1.30 \(\times\) 10\(^6\) Pa at 22.0\(^\circ\)C. The temperature of the gas remains constant as it is partially emptied out of the tank, until the gauge pressure is 3.40 \(\times\) 10\(^5\) Pa. Calculate the mass of propane that has been used.

A 20.0-L tank contains \(4.86 \times 10{^-}{^4}\) kg of helium at 18.0\(^\circ\)C. The molar mass of helium is 4.00 g/mol. (a) How many moles of helium are in the tank? (b) What is the pressure in the tank, in pascals and in atmospheres?

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