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Construct a concept map to show the interrelationships between path-dependent and pathindependent quantities in thermodynamics.

Short Answer

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A concept map has been drawn to show the interrelationships of path-dependent quantities like heat and work, and path-independent quantities like internal energy, enthalpy, and entropy in thermodynamics. The map illustrates that path-independent quantities measure the equilibrium state properties while path-dependent quantities describe the process of change from one state to another.

Step by step solution

01

Define concepts

Start by defining path-dependent and path-independent quantities. Path-dependent quantities are the ones where the final state depends on the path taken to get there. An example of this in thermodynamics would be heat and work. Path-independent quantities, on the other hand, only depend on the initial and final states regardless of the path. In thermodynamics, internal energy, enthalpy, and entropy are examples of path-independent quantities.
02

Draw the map

Begin to draw the concept map by placing 'Thermodynamics' at the center. Around it, write 'Path-dependent quantities' and 'Path-independent quantities'. Draw lines connecting 'Thermodynamics' to these two terms.
03

Add examples

On the 'Path-dependent quantities' side, add 'work' and 'heat', while on the 'Path-independent quantities' side, add 'internal energy', 'enthalpy', and 'entropy'.
04

Show interrelationships

To show the interrelationships, add a new branch named 'Interactions'. Point out that path-independent quantities measure the equilibrium state properties while path-dependent quantities describe the process of change from one state to another. This interaction is crucial in understanding how energy is transferred or transformed in thermodynamic systems.

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Key Concepts

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

Path-Dependent Quantities
In the realm of thermodynamics, comprehending path-dependent quantities is crucial for understanding how energy transitions occur. These are variables whose values are reliant on the specific route taken during a process. For example, work and heat are classic path-dependent quantities.

Imagine you're hiking up a mountain; the distance you travel and the work you do depend on whether you take a steep shortcut or a longer, winding path. Similarly, if a gas expands in a cylinder, the work done by or on the gas is path-dependent. The energy imparted, through heat, to bring about this change also varies with the different processes the gas might undergo.

Therefore, path-dependent quantities tell the story of the journey from initial to final states. They are contingent on the sequence of intermediate states and inherently describe energy changes during transitions, which is pivotal in processes such as heating, cooling, or mechanical work.
Path-Independent Quantities
Conversely, path-independent quantities are the constants in the story of thermodynamics. They are properties of the system that are determined solely by the initial and final states, irrespective of the way those states were reached. Principal examples include internal energy, enthalpy, and entropy.

To visualize, think of your final altitude on that mountain peak; it doesn't matter which path you took, the height above sea level is the same at the top. In thermodynamic systems, whether a gas reaches a certain energy state through heating or mechanical work, the internal energy will be the same for the same final conditions.

These quantities are essential for defining the equilibrium state of a system and for applying conservation principles, like the first law of thermodynamics, which asserts that energy can neither be created nor destroyed in an isolated system.
Concept Map in Thermodynamics
Creating a concept map is an effective educational tool to organize and visualize the relationships between different concepts in thermodynamics. Starting at the center with Thermodynamics, we branch out to Path-dependent quantities and Path-independent quantities, which form the fundamental groups.

Developing the Map

As we develop the map, we attach examples like 'work' and 'heat' to the path-dependent side, whereas 'internal energy', 'enthalpy', and 'entropy' are linked to the path-independent side. Linking these concepts reveals a structured understanding of how thermodynamic properties interact and affect each other.

Additionally, concept maps are in themselves path-independent tools for learning—they lead to a comprehensive grasp of the subject no matter the starting point of the learning process.
Thermodynamics Equilibrium State
The state of thermodynamic equilibrium is a key concept that denotes a system's balance. At this juncture, there are no unbalanced potentials, or driving forces, within the system; meaning that no macroscopic changes can occur.

This equilibrium can be categorized into different types, such as thermal, mechanical, and chemical equilibrium. Thermal equilibrium ensures that there is no heat flow within the system or between the system and its environment. Mechanical equilibrium means that there is no change in pressure at any point of the system, and likewise, chemical equilibrium indicates no chemical reactions are occurring or, if they are, they are proceeding at equal and opposite rates.

In essence, when we speak of path-independent quantities, we are often describing the properties of a system that is in or moving towards a state of thermodynamic equilibrium. This state is fundamental to the study and practical application of thermodynamics because it allows us to set reference points and predict how systems will behave under certain conditions.

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Most popular questions from this chapter

Explain the important distinctions between each pair of terms: (a) system and surroundings; (b) heat and work; (c) specific heat and heat capacity; (d) endothermic and exothermic; (e) constant-volume process and constant-pressure process.

The internal energy of a fixed quantity of an ideal gas depends only on its temperature. A sample of an ideal gas is allowed to expand at a constant temperature (isothermal expansion). (a) Does the gas do work? (b) Does the gas exchange heat with its surroundings? (c) What happens to the temperature of the gas? (d) What is \(\Delta U\) for the gas?

What will be the final temperature of the water in an insulated container as the result of passing \(5.00 \mathrm{g}\) of steam, \(\mathrm{H}_{2} \mathrm{O}(\mathrm{g}),\) at \(100.0^{\circ} \mathrm{C}\) into \(100.0 \mathrm{g}\) of water at \(25.0^{\circ} \mathrm{C} ?\left(\Delta H_{\mathrm{vap}}^{\circ}=40.6 \mathrm{kJ} / \mathrm{mol} \mathrm{H}_{2} \mathrm{O}\right)\).

One glucose molecule, \(\mathrm{C}_{6} \mathrm{H}_{12} \mathrm{O}_{6}(\mathrm{s}),\) is converted to two lactic acid molecules, \(\mathrm{CH}_{3} \mathrm{CH}(\mathrm{OH}) \mathrm{COOH}(\mathrm{s})\) during glycolysis. Given the combustion reactions of glucose and lactic acid, determine the standard enthalpy for glycolysis. $$\begin{array}{r} \mathrm{C}_{6} \mathrm{H}_{12} \mathrm{O}_{6}(\mathrm{s})+6 \mathrm{O}_{2}(\mathrm{g}) \longrightarrow 6 \mathrm{CO}_{2}(\mathrm{g})+6 \mathrm{H}_{2} \mathrm{O}(\mathrm{l}) \\ \Delta H^{\circ}=-2808 \mathrm{kJ} \end{array}$$ $$\begin{aligned} \mathrm{CH}_{3} \mathrm{CH}(\mathrm{OH}) & \mathrm{COOH}(\mathrm{s})+3 \mathrm{O}_{2}(\mathrm{g}) \longrightarrow \\ 3 \mathrm{CO}_{2}(\mathrm{g})+3 \mathrm{H}_{2} \mathrm{O}(1) & \Delta H^{\circ}=-1344 \mathrm{kJ} \end{aligned}$$

How much heat, in kilojoules, is associated with the production of \(283 \mathrm{kg}\) of slaked lime, \(\mathrm{Ca}(\mathrm{OH})_{2} ?\) $$\mathrm{CaO}(\mathrm{s})+\mathrm{H}_{2} \mathrm{O}(1) \longrightarrow \mathrm{Ca}(\mathrm{OH})_{2}(\mathrm{s}) \quad \Delta H^{\circ}=-65.2 \mathrm{kJ}$$

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