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You have a 1.00 -L sample of hot water \(\left(90.0^{\circ} \mathrm{C}\right)\) sitting open in a \(25.0^{\circ} \mathrm{C}\) room. Eventually the water cools to \(25.0^{\circ} \mathrm{C}\) while the temperature of the room remains unchanged. Calculate \(\Delta S_{\mathrm{sur}}\) for this process. Assume the density of water is 1.00 \(\mathrm{g} / \mathrm{cm}^{3}\) over this temperature range, and the heat capacity of water is constant over this temperature range and equal to 75.4 \(\mathrm{J} / \mathrm{K} \cdot\) mol.

Short Answer

Expert verified
The change in entropy of the surroundings, \(\Delta S_{\text{sur}}\), for the process of hot water cooling to room temperature is 871.6 J/K.

Step by step solution

01

Find the number of moles of water

First, you need to find the number of moles of water in the 1.00 L sample. Use the density of water, 1.00 g/cm³, to do this. Since 1 L = 1000 cm³, you have: Mass of water = Volume × Density = 1000 cm³ × 1.00 g/cm³ = 1000 g Now, find the number of moles of water, knowing that the molar mass of water is 18.02 g/mol: Number of moles = Mass / Molar mass = 1000 g / 18.02 g/mol = 55.49 mol
02

Calculate the heat exchanged

Now, calculate the amount of heat released by the water as it cools down from 90.0°C to 25.0°C. Use the heat capacity of water and the temperature difference: \(q = n \times C \times \Delta T\) \(q = 55.49 \mathrm{mol} \times 75.4 \mathrm{\frac{J}{K \cdot mol}} \times (25.0 ^\circ \mathrm{C} - 90.0 ^\circ \mathrm{C})\) \(q = 55.49 \mathrm{mol} \times 75.4 \mathrm{\frac{J}{K \cdot mol}} \times -65.0 \mathrm{K}\) \(q = -259910.3 \mathrm{J}\) The heat exchanged (q) is negative because it was released to the surroundings by the water sample.
03

Calculate the change in entropy of the surroundings

Finally, calculate the change in entropy of the surroundings with the formula: \(\Delta S_{\text{sur}} = -\frac{q}{T}\) Since the temperature of the room remains constant at 25.0°C, you can use that in the formula, but you need to convert it to Kelvin first: 25.0°C + 273.15 = 298.15 K \(\Delta S_{\text{sur}} = -\frac{-259910.3 \mathrm{J}}{298.15 \mathrm{K}}\) \(\Delta S_{\text{sur}} = 871.6 \mathrm{\frac{J}{K}}\) The change in entropy of the surroundings, \(\Delta S_{\text{sur}}\), is 871.6 J/K.

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Key Concepts

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

Water Cooling
Water cooling is a natural process where the water's temperature decreases until it reaches equilibrium with its surroundings. In this scenario, the sample starts at 90°C and gradually adjusts to the room temperature of 25°C. This process is crucial for understanding thermodynamics, as it exemplifies energy transfer. The cooling of water involves releasing heat to the surroundings until an equal temperature is reached, demonstrating the principle of heat exchange.
The cooling effect can be observed not only in everyday experiences but also in industrial settings where controlled cooling is necessary for various processes. It is also essential for understanding concepts such as entropy and heat capacity, which dictate energy distribution in any given system. Understanding water cooling helps students grasp larger principles of physics and chemistry, grounding theoretical knowledge in practical, observable phenomena.
Heat Capacity
Heat capacity is a measure of the amount of heat energy required to change a substance's temperature by a certain amount. In this example, the heat capacity of water is given as 75.4 J/K·mol. This value tells us how much energy, in joules, is necessary to raise the temperature of one mole of water by one degree Kelvin.
Heat capacity is an intrinsic property, meaning it is specific to each material. For water, known for its relatively high heat capacity, this feature explains why it can absorb or release large amounts of heat without experiencing quick temperature changes.
  • The high heat capacity of water is crucial for moderating Earth's climate and biological systems.
  • When calculating thermal changes in systems, understanding heat capacity allows accurate predictions of how substances will react to energy input or removal.
By grasping heat capacity, students can better understand and predict the behavior of substances under various thermal conditions.
Number of Moles
The number of moles is a fundamental concept in chemistry that represents a specific quantity of substance. It helps in quantifying the amount of molecules or atoms in a given sample. For the water sample in this exercise, the number of moles is calculated using its mass and the molar mass of water, 18.02 g/mol. First, the mass of water is determined as 1000 g since we know 1 L of water weighs about 1000 g.
Next, dividing this mass by the molar mass of water gives us approximately 55.49 moles. Understanding moles is essential for balancing chemical equations, calculating concentrations, and performing various stoichiometric calculations in chemistry.
  • Moles bridge the gap between atomic-scale properties and macroscopic measurements we can observe.
  • They simplify complex interactions into understandable proportions.
Recognizing how to compute and use moles empowers students to explore deeper chemical relationships and interactions.
Heat Exchange
Heat exchange describes the energy transfer between a system and its surroundings. In our example, heat transfer occurs when hot water releases thermal energy into the cooler surrounding air, resulting in the water's temperature dropping. The magnitude of this heat exchange can be calculated using the formula:\( q = n \times C \times \Delta T \)Here, 'q' represents the heat exchanged, 'n' stands for the number of moles, 'C' is the heat capacity, and \( \Delta T \) signifies the temperature change.
In this scenario, the negative sign of \( q \) confirms that energy leaves the water as it cools. Understanding heat exchange is pivotal in thermodynamics, where energy conservation and transformation are key principles.
  • Heat exchange impacts various processes, from everyday cooking to industrial cooling systems.
  • It illustrates the flow of energy and contributes to understanding entropy—a measure of disorder within a system.
Mastering this concept allows students to comprehend energy transfer processes, equipping them with insights into both simple and sophisticated thermal systems.

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Most popular questions from this chapter

For mercury, the enthalpy of vaporization is 58.51 kJ/mol and the entropy of vaporization is 92.92 J/K ? mol. What is the normal boiling point of mercury?

It is quite common for a solid to change from one structure to another at a temperature below its melting point. For example, sulfur undergoes a phase change from the rhombic crystal structure to the monoclinic crystal form at temperatures above \(95^{\circ} \mathrm{C}\) a. Predict the signs of \(\Delta H\) and \(\Delta S\) for the process \(\mathrm{S}_{\text { rhombic}}(s)\longrightarrow \mathrm{S}_{\text { monoclinic }}(s)\) b. Which form of sulfur has the more ordered crystalline structure (has the smaller positional probability)?

Impure nickel, refined by smelting sulfide ores in a blast furnace, can be converted into metal from 99.90% to 99.99% purity by the Mond process. The primary reaction involved in the Mond process is $$\mathrm{Ni}(s)+4 \mathrm{CO}(g) \rightleftharpoons \mathrm{Ni}(\mathrm{CO})_{4}(g)$$ a. Without referring to Appendix \(4,\) predict the sign of \(\Delta S^{\circ}\) for the above reaction. Explain. b. The spontaneity of the above reaction is temperature-dependent. Predict the sign of \(\Delta S_{\text { sum }}\) for this reaction. Explain. c. For \(\mathrm{Ni}(\mathrm{CO})_{4}(g), \Delta H_{\mathrm{f}}^{\circ}=-607 \mathrm{kJ} / \mathrm{mol}\) and \(S^{\circ}=417 \mathrm{J} / \mathrm{K} \cdot \mathrm{mol}\) at 298 \(\mathrm{K}\) . Using these values and data in Appendix 4 calculate \(\Delta H^{\circ}\) and \(\Delta S^{\circ}\) for the above reaction. d. Calculate the temperature at which \(\Delta G^{\circ}=0(K=1)\) for the above reaction, assuming that \(\Delta H^{\circ}\) and \(\Delta S^{\circ}\) do not depend on temperature. e. The first step of the Mond process involves equilibrating impure nickel with \(\mathrm{CO}(g)\) and \(\mathrm{Ni}(\mathrm{CO})_{4}(g)\) at about \(50^{\circ} \mathrm{C} .\) The purpose of this step is to convert as much nickel as possible into the gas phase. Calculate the equilibrium constant for the above reaction at \(50 .^{\circ} \mathrm{C}\) f. In the second step of the Mond process, the gaseous \(\mathrm{Ni}(\mathrm{CO})_{4}\) is isolated and heated to \(227^{\circ} \mathrm{C}\) . The purpose of this step is to deposit as much nickel as possible as pure solid (the reverse of the preceding reaction). Calculate the equilibrium constant for the preceding reaction at \(227^{\circ} \mathrm{C}\) . g. Why is temperature increased for the second step of the Mond process? h. The Mond process relies on the volatility of \(\mathrm{Ni}(\mathrm{CO})_{4}\) for its success. Only pressures and temperatures at which \(\mathrm{Ni}(\mathrm{CO})_{4}\) is a gas are useful. A recently developed variation of the Mond process carries out the first step at higher pressures and a temperature of \(152^{\circ} \mathrm{C}\) . Estimate the maximum pressure of \(\mathrm{Ni}(\mathrm{CO})_{4}(g)\) that can be attained before the gas will liquefy at \(152^{\circ} \mathrm{C}\) . The boiling point for Nic CO) is \(42^{\circ} \mathrm{C}\) and the enthalpy of vaporization is 29.0 \(\mathrm{kJ} / \mathrm{mol} .\) [Hint: The phase change reaction and the corresponding equilibrium expression are \(\mathrm{Ni}(\mathrm{CO})_{4}(l) \rightleftharpoons \mathrm{Ni}(\mathrm{CO})_{4}(g) \quad K=P_{\mathrm{NiCO} 4}\) greater than the \(K\) value. \(]\)

Hydrogen cyanide is produced industrially by the following exothermic reaction: $$2 \mathrm{NH}_{3}(g)+3 \mathrm{O}_{2}(g)+2 \mathrm{CH}_{4}(g) \longrightarrow 2 \mathrm{HCN}(g)+6 \mathrm{H}_{2} \mathrm{O}(g)$$ Is the high temperature needed for thermodynamic or kinetic reasons?

Consider two perfectly insulated vessels. Vessel 1 initially contains an ice cube at \(0^{\circ} \mathrm{C}\) and water at \(0^{\circ} \mathrm{C}\) . Vessel 2 initially contains an ice cube at \(0^{\circ} \mathrm{C}\) and a saltwater solution at \(0^{\circ} \mathrm{C}\) . Consider the process \(\mathrm{H}_{2} \mathrm{O}(s) \rightarrow \mathrm{H}_{2} \mathrm{O}(l)\) a. Determine the sign of \(\Delta S, \Delta S_{\text { sum }}\) and \(\Delta S_{\text { univ }}\) for the process in vessel 1 . b. Determine the sign of \(\Delta S, \Delta S_{\text { sum }},\) and \(\Delta S_{\text { univ }}\) for the process in vessel \(2 .\) (Hint: Think about the effect that a salt has on the freezing point of a solvent.)

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