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Ch 19: The First Law of Thermodynamics
Young & Freedman Calc - University Physics 15th Edition
Young & Freedman Calc15th EditionUniversity PhysicsISBN: 9780135159552Not the one you use?Change textbook
Chapter 19, Problem 14b

When water is boiled at a pressure of 2.002.00 atm, the heat of vaporization is 2.20×1062.20\(\times\)10^6 J/kg and the boiling point is 120120°C. At this pressure, 1.001.00 kg of water has a volume of 1.00×1031.00\(\times\)10^{-3} m3, and 1.001.00 kg of steam has a volume of 0.8240.824 m3. Compute the increase in internal energy of the water.

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Identify the given values: pressure (P) = 2.00 atm, heat of vaporization (L) = 2.20 * 10^6 J/kg, initial volume of water (V1) = 1.00 * 10^-3 m^3, final volume of steam (V2) = 0.824 m^3, and mass (m) = 1.00 kg.
Convert the pressure from atm to pascals (Pa) using the conversion factor: 1 atm = 1.013 * 10^5 Pa. Therefore, P = 2.00 * 1.013 * 10^5 Pa.
Calculate the work done (W) during the expansion using the formula: W = P * (V2 - V1). Substitute the values for P, V2, and V1 to find the work done.
Use the first law of thermodynamics to find the change in internal energy (ΔU): ΔU = Q - W, where Q is the heat added to the system. Here, Q is equal to the heat of vaporization multiplied by the mass, Q = L * m.
Substitute the values of Q and W into the equation ΔU = Q - W to find the increase in internal energy of the water.

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Key Concepts

Here are the essential concepts you must grasp in order to answer the question correctly.

Heat of Vaporization

The heat of vaporization is the amount of energy required to convert a unit mass of a liquid into vapor without a temperature change. For water at 2.00 atm, this value is 2.20 * 10^6 J/kg. It is crucial for calculating the energy needed to vaporize water and understanding phase transitions.
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First Law of Thermodynamics

The First Law of Thermodynamics states that energy cannot be created or destroyed, only transformed. It is expressed as ΔU = Q - W, where ΔU is the change in internal energy, Q is the heat added to the system, and W is the work done by the system. This principle helps calculate the change in internal energy when water boils.
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Work Done by Expanding Gas

When a gas expands, it does work on its surroundings, calculated as W = PΔV, where P is the pressure and ΔV is the change in volume. In this scenario, the work done by the steam as it expands from liquid to gas at 2.00 atm is essential for determining the internal energy change during boiling.
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Related Practice
Textbook Question

A cylinder contains 0.01000.0100 mol of helium at T=27.0T = 27.0°C. If instead the pressure of the helium is kept constant, how much heat is needed to raise the temperature from 27.027.0°C to 67.067.0°C? Draw a pVpV-diagram for this process.

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Textbook Question

A gas in a cylinder is held at a constant pressure of 1.80×1051.80\(\times\)10^5 Pa and is cooled and compressed from 1.701.70 m3 to 1.201.20 m3. The internal energy of the gas decreases by 1.40×1051.40\(\times\)10^5 J. Does it matter whether the gas is ideal? Why or why not?

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Textbook Question

During an isothermal compression of an ideal gas, 410410 J of heat must be removed from the gas to maintain constant temperature. How much work is done by the gas during the process?

Textbook Question

The pVpV-diagram in Fig. E19.1319.13 shows a process abcabc involving 0.4500.450 mol of an ideal gas. How much heat had to be added during the process to increase the internal energy of the gas by 15,00015,000 J?

1
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Textbook Question

A cylinder contains 0.01000.0100 mol of helium at T=27.0T = 27.0°C. How much heat is needed to raise the temperature to 67.067.0°C while keeping the volume constant? Draw a pVpV-diagram for this process.

1
views
Textbook Question

When water is boiled at a pressure of 2.002.00 atm, the heat of vaporization is 2.20×1062.20\(\times\)10^6 J/kg and the boiling point is 120120°C. At this pressure, 1.001.00 kg of water has a volume of 1.00×1031.00\(\times\)10^{-3} m3, and 1.001.00 kg of steam has a volume of 0.8240.824 m3. Compute the work done when 1.001.00 kg of steam is formed at this temperature.

1
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