Problem 2
Question
Which of the following is not a thermodynamic property of a system? (a) \(H\) (b) \(P\) (c) \(E\) (d) w
Step-by-Step Solution
Verified Answer
(d) w is not a thermodynamic property of a system; it's a path function.
1Step 1: Understanding Thermodynamic Properties
Thermodynamic properties are characteristics that define the state of a system in equilibrium. Common examples include pressure (P), volume (V), temperature (T), and enthalpy (H). These properties are state functions which means they depend only on the current state of the system, not on the path the system took to reach that state.
2Step 2: Identify State Functions and Path Functions
State functions include properties like enthalpy (H), pressure (P), and internal energy (E). These do not depend on the process the system undergoes. Path functions, on the other hand, depend on the path taken by the system from the initial to the final state. Work (w) and heat (q) are examples of path functions, as they describe the energy transfer, not the state of the system.
3Step 3: Evaluate the Given Options
Looking at the provided options, we see that (a) H is enthalpy, (b) P is pressure, and (c) E represents internal energy. These are all state functions. Option (d) w represents work, which is a path function, not a thermodynamic property (state function).
Key Concepts
Enthalpy (H)Pressure (P)Internal Energy (E)Path Function vs State Function
Enthalpy (H)
Enthalpy, symbolized by the letter H, is a measure of the total heat content in a thermodynamic system. It encompasses both the internal energy (E) of the system and the energy needed to make room for it by displacing its environment, considering the system's pressure (P) and volume (V). Enthalpy is defined by the equation:
\[ H = E + PV \].
It is a crucial concept when dealing with heat transfer during chemical reactions, particularly in constant pressure situations, often encountered in chemistry. When a reaction releases heat, it is exothermic, and the change in enthalpy (\triangle H) is negative. Conversely, when the system absorbs heat, the reaction is endothermic, and \triangle H is positive. The ease of measuring enthalpy changes makes it a valuable tool for understanding the energy changes that occur in reactions.
\[ H = E + PV \].
It is a crucial concept when dealing with heat transfer during chemical reactions, particularly in constant pressure situations, often encountered in chemistry. When a reaction releases heat, it is exothermic, and the change in enthalpy (\triangle H) is negative. Conversely, when the system absorbs heat, the reaction is endothermic, and \triangle H is positive. The ease of measuring enthalpy changes makes it a valuable tool for understanding the energy changes that occur in reactions.
Pressure (P)
Pressure is a fundamental thermodynamic property represented by the symbol P. It is defined as the force exerted per unit area on the walls of a container by the particles (atoms or molecules) within a system.
Pressure plays a pivotal role in understanding how systems react to external changes. For instance, gas pressure can be explained using the Ideal Gas Law:
\[ PV = nRT \],
where P stands for pressure, V is the volume, n represents the number of moles, R is the gas constant, and T is temperature. This relation shows that pressure is directly proportional to temperature and the number of particles, but inversely proportional to volume. Pressure measurements are essential for various applications, from predicting the weather (atmospheric pressure) to explaining the behavior of gases in closed systems.
Pressure plays a pivotal role in understanding how systems react to external changes. For instance, gas pressure can be explained using the Ideal Gas Law:
\[ PV = nRT \],
where P stands for pressure, V is the volume, n represents the number of moles, R is the gas constant, and T is temperature. This relation shows that pressure is directly proportional to temperature and the number of particles, but inversely proportional to volume. Pressure measurements are essential for various applications, from predicting the weather (atmospheric pressure) to explaining the behavior of gases in closed systems.
Internal Energy (E)
Internal energy (E) is the sum of all the energy contained within a system. It consists of the kinetic energy due to the movement of particles, and potential energy resulting from force interactions among these particles, such as chemical bonds.
Internal energy is a key player in the First Law of Thermodynamics, which states that energy cannot be created or destroyed in an isolated system, only transferred or transformed. Mathematically expressed as:
\[ \triangle E = q + w \],
\triangle E represents the change in internal energy, q stands for heat exchanged with the surroundings, and w is the work done by or on the system. The concept of internal energy is vital because it links to other properties like enthalpy and provides insights on how energy transfer influences physical changes within a system.
Internal energy is a key player in the First Law of Thermodynamics, which states that energy cannot be created or destroyed in an isolated system, only transferred or transformed. Mathematically expressed as:
\[ \triangle E = q + w \],
\triangle E represents the change in internal energy, q stands for heat exchanged with the surroundings, and w is the work done by or on the system. The concept of internal energy is vital because it links to other properties like enthalpy and provides insights on how energy transfer influences physical changes within a system.
Path Function vs State Function
The distinction between a path function and a state function is vital in the realm of thermodynamics. A state function is a property whose value only depends on the current state of the system, regardless of how the system arrived there. Examples include enthalpy (H), pressure (P), and internal energy (E), and these can be compared to geographical locations on a map—no matter the path you took, your destination is the same.
Conversely, path functions are properties that depend on the route taken from the initial to the final state. They describe how a process occurs rather than the state of the system. Work (w) and heat (q) are path functions because the amount of work done or heat transferred can vary greatly depending on the path followed. This concept is analogous to the distance traveled—it matters whether you took the scenic route or the highway. Understanding the difference aids in solving problems related to heat transfer, work, and state properties of systems.
Conversely, path functions are properties that depend on the route taken from the initial to the final state. They describe how a process occurs rather than the state of the system. Work (w) and heat (q) are path functions because the amount of work done or heat transferred can vary greatly depending on the path followed. This concept is analogous to the distance traveled—it matters whether you took the scenic route or the highway. Understanding the difference aids in solving problems related to heat transfer, work, and state properties of systems.
Other exercises in this chapter
Problem 3
An average human produces about \(10 \mathrm{MJ}\) of heat each day through metabolic activity. If a human body were an isolated system of mass \(80 \mathrm{~kg
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The heat capacity of liquid water is \(75.6 \mathrm{~J} / \mathrm{K}-\mathrm{mol}\), while the enthalpy of fusion of ice is \(6.0 \mathrm{~kJ} / \mathrm{mol}\).
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An insulated container of gas has two chambers separated by an insulating partition. One of the chambers has volume \(V_{1}\) and contains an ideal gas at press
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