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(a) Which of the following cannot leave or enter a closed system: heat, work, or matter? (b) Which cannot leave or enter an isolated system? (c) What do we call the part of the universe that is not part of the system?

Short Answer

Expert verified
(a) In a closed system, "matter" cannot leave or enter the system. (b) In an isolated system, "heat, work, and matter" cannot leave or enter the system. (c) The part of the universe that is not part of the system is called the "surroundings."

Step by step solution

01

(a) Closed System: Definition

A closed system is one in which mass (matter) cannot enter or leave the system but energy (heat and work) can be transferred across its boundary.
02

(a) Closed System: Identification

In a closed system, matter cannot leave or enter the system. Therefore, the answer for part (a) is "matter."
03

(b) Isolated System: Definition

An isolated system is one in which neither mass nor energy can be transferred across its boundary. It is completely separated from its surroundings.
04

(b) Isolated System: Identification

In an isolated system, no heat, work, or matter can leave or enter the system. Therefore, the answer for part (b) is "heat, work, and matter."
05

(c) Universe: System and Surroundings

In thermodynamics, the universe consists of two parts: the system under study and the surroundings. The surroundings encompass everything else that lies outside the system and can interact with it.
06

(c) Universe: Terminology

We call the part of the universe that is not part of the system the "surroundings."

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Key Concepts

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

Closed System
A closed system is a fundamental concept in thermodynamics. It describes a system where no matter can enter or leave. This might sound a bit limiting, but energy can still cross the boundaries. This includes both heat and work.

Here's how it works:
  • No exchange of matter: The mass within the system remains constant at all times. So, if a scenario describes a system without any matter coming in or going out, it is likely closed.
  • Energy exchange: Energy is free to move in and out, either in the form of heat or work. This allows for many dynamic processes to happen, even within the closed boundaries.
In practical examples, think of a closed water bottle. You can't pour more water in or out without opening the cap, but if the bottle is exposed to the sun, it might heat up due to energy transfer.
Isolated System
An isolated system takes things a step further than a closed system. In this type of system, neither matter nor energy can cross the boundaries. It is completely insulated and separated from its surroundings.

Characteristics of an isolated system include:
  • No matter exchange: Just like a closed system, no matter goes in or out.
  • No energy exchange: Unlike a closed system, even energy in the form of heat or work cannot be transferred across its boundaries.
An easy way to remember this is to think of an ideal thermos flask. An ideal thermos would not allow the heat to escape or enter, keeping your drink at the same temperature, no matter what's happening outside.
Surroundings
The surroundings refer to everything that is outside of the system being studied in thermodynamics. When considering problems in thermodynamics, we often describe the system and then everything else that it's interacting with as the surroundings.

Important points about surroundings:
  • The surroundings can interact with the system, affecting or being affected by energy or matter transfer, depending on the system’s classification (closed, open, or isolated).
  • Understanding surroundings helps to predict how the system will behave. For instance, if a system is transferring heat to its surroundings, the temperature might change accordingly.
Imagine you were testing a car engine (the system). The air, road, and even the environment around the car would be considered as the surroundings.

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Most popular questions from this chapter

A coffee-cup calorimeter of the type shown in Figure 5.18 contains \(150.0 \mathrm{~g}\) of water at \(25.2^{\circ} \mathrm{C}\). A \(200-\mathrm{g}\) block of silver metal is heated to \(100.5^{\circ} \mathrm{C}\) by putting it in a beaker of boiling water. The specific heat of \(\mathrm{Ag}(s)\) is \(0.233 \mathrm{~J} /(\mathrm{g} \cdot \mathrm{K})\). The \(\mathrm{Ag}\) is added to the calorimeter, and after some time the contents of the cup reach a constant temperature of \(30.2^{\circ} \mathrm{C} .(\mathbf{a})\) Determine the amount of heat, in J, lost by the silver block. (b) Determine the amount of heat gained by the water. The specific heat of water is \(4.184 \mathrm{~J} /(\mathrm{g} \cdot \mathrm{K}) .(\mathbf{c})\) The difference between your answers for (a) and (b) is due to heat loss through the Styrofoam \(^{\circ}\) cups and the heat necessary to raise the temperature of the inner wall of the apparatus. The heat capacity of the calorimeter is the amount of heat necessary to raise the temperature of the apparatus (the cups and the stopper) by \(1 \mathrm{~K} .\) Calculate the heat capacity of the calorimeter in \(\mathrm{J} / \mathrm{K}\). (d) What would be the final temperature of the system if all the heat lost by the silver block were absorbed by the water in the calorimeter?

(a) A serving of a particular ready-to-serve brown \& wild rice meal contains \(4.5 \mathrm{~g}\) fat, \(42 \mathrm{~g}\) carbohydrate, and \(4.0 \mathrm{~g}\) protein. Estimate the number of calories in a serving. (b) According to its nutrition label, the same meal also contains \(140 \mathrm{mg}\) of potassium ions. Do you think the potassium contributes to the caloric content of the food?

(a) What is meant by the term standard conditions with reference to enthalpy changes? (b) What is meant by the term enthalpy of formation? (c) What is meant by the term standard enthalpy of formation?

(a) What is meant by the term state function? (b) Give an example of a quantity that is a state function and one that is not. (c) Is the volume of a system a state function? Why or why not?

Complete combustion of 1 mol of acetone \(\left(\mathrm{C}_{3} \mathrm{H}_{6} \mathrm{O}\right)\) liberates \(1790 \mathrm{~kJ}:\) $$ \begin{aligned} \mathrm{C}_{3} \mathrm{H}_{6} \mathrm{O}(l)+4 \mathrm{O}_{2}(g) \longrightarrow 3 \mathrm{CO}_{2}(g)+3 \mathrm{H}_{2} \mathrm{O}(l) & \\ \Delta H^{\circ}=&-1790 \mathrm{~kJ} \end{aligned} $$ Using this information together with the standard enthalpies of formation of \(\mathrm{O}_{2}(g), \mathrm{CO}_{2}(g),\) and \(\mathrm{H}_{2} \mathrm{O}(l)\) from Appendix C, calculate the standard enthalpy of formation of acetone.

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