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What is the relation \(h_{\text {heat }}=\rho c_{p} h_{\text {mass }}\) known as? For what kind of mixtures is it valid? What is the practical importance of it?

Short Answer

Expert verified
Answer: The practical importance of the thermal enthalpy-volume relationship lies in its application within engineering calculations and designing heat exchangers or cooling systems. For incompressible substances, this relation simplifies the calculations and helps in analyzing heat transfer processes in various industrial applications. It is essential for engineers and scientists working in the fields of thermodynamics, heat transfer, and energy systems.

Step by step solution

01

Identifying the relation and its terms

The given relation is \(h_{\text {heat }}=\rho c_{p} h_{\text {mass }}\), where: - \(h_{\text {heat }}\) is the specific enthalpy, which is the energy per unit mass associated with heat transfer; - \(\rho\) is the density of the substance, representing its mass per unit volume; - \(c_{p}\) is the heat capacity at constant pressure, which is the amount of heat required to raise the temperature of one unit mass of the substance by one degree Celsius or Kelvin; - \(h_{\text {mass }}\) is usually known as specific volume, which is the volume per unit mass of the substance. It is the reciprocal of density (\(h_{\text {mass }} = \frac{1}{\rho}\)).
02

Understanding the relation's validity

The relation \(h_{\text {heat }}=\rho c_{p} h_{\text {mass }}\) is known as the "thermal enthalpy-volume relationship". It is valid for incompressible substances, where the density remains constant throughout the process. Incompressible substances have small changes in volume during the process, and typically these are liquids and solids at moderate temperatures and pressures.
03

Discussing the practical importance of the relation

The practical importance of the thermal enthalpy-volume relationship lies in its application within engineering calculations and designing heat exchangers or cooling systems. For incompressible substances, this relation simplifies the calculations and helps in analyzing heat transfer processes in various industrial applications. Consequently, it is essential for engineers and scientists working in the fields of thermodynamics, heat transfer, and energy systems.

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Key Concepts

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

Specific Enthalpy
Specific enthalpy, denoted usually as \( h \), is a key concept in thermodynamics that refers to the total energy per unit mass of a substance, including both its internal energy and the energy associated with the pressure of the substance. It plays a pivotal role in calculating the heat transfer during a thermodynamic process.

For instance, when a fluid undergoes a process that involves heating or cooling, the change in specific enthalpy can help determine the amount of heat transferred, assuming no work is done by or on the system. It's instrumental in various engineering applications, such as determining the energy efficiency of heat exchangers and performing energy balance calculations.

The formula \(h_{\text{heat}} = \rho c_{p} h_{\text{mass}}\), with specific enthalpy represented by \(h_{\text{heat}}\), density by \(\rho\), and heat capacity at constant pressure by \(c_{p}\), makes it easier to compute energy changes during heat transfer in incompressible substances.
Heat Capacity
Heat capacity, often symbolized as \( c_{p} \) when it's measured at constant pressure, is the amount of heat required to raise the temperature of a unit mass of a substance by one degree Celsius or Kelvin. It essentially indicates how much energy you need to pump into a substance to increase its temperature, which is vital for designing thermal systems.

Different substances have varying heat capacities, which allows scientists and engineers to select materials based on how efficiently they can store or transfer heat. For example, water has a high heat capacity, making it an effective coolant. The relation \(h_{\text{heat}} = \rho c_{p} h_{\text{mass}}\) incorporates heat capacity to correlate the energy change to both the material's properties and the heat transfer process involved.
Density
Density, represented by \( \rho \), is a fundamental property of matter that indicates mass per unit volume. It's crucial in various fields, from material science to fluid dynamics.

In the context of the thermal enthalpy-volume relationship, \( \rho \), or density, helps determine how much specific enthalpy a certain volume of a substance can contain. Higher density means more mass in a given volume, which could lead to a larger amount of heat transfer in that volume. Understanding density allows for precise calculations in applications where mass and volume work together to affect energy distribution, such as in heating systems or refrigerators.
Specific Volume
Specific volume, denoted by \( h_{\text{mass}} \) in the given relation, is essentially the inverse of density. While density measures mass per unit volume, specific volume measures the volume that one unit of mass occupies. It is critical when dealing with gases where changes in pressure and temperature significantly affect volume.

In practical applications, knowing the specific volume helps engineers design systems with appropriate dimensions to contain gases or liquids at different stages of thermal processes, ensuring efficiency and safety. The use of specific volume in the thermal enthalpy-volume relationship simplifies calculations because it provides a direct measure that can be easily manipulated mathematically.
Incompressible Substances
Incompressible substances are characterized by their negligible change in volume when subjected to pressure. Common examples include liquids and solids under typical conditions. Due to their nearly constant density, the thermal enthalpy-volume relationship can be reliably applied to them.

When dealing with incompressible substances, you can assume their density remains the same while analyzing thermal processes. This assumption streamlines the mathematics involved and is useful in various practical scenarios, such as plumbing design, where water (an incompressible fluid) is often the working substance.
Heat Transfer
Heat transfer is the movement of thermal energy from one body or substance to another. It can occur through conduction, convection, or radiation, and understanding it is fundamental in designing and analyzing heating and cooling systems.

The thermal enthalpy-volume relationship is a valuable tool for quantifying heat transfer in incompressible substances. By incorporating properties like specific enthalpy, density, and specific volume, this relationship enables the prediction and analysis of how heat energy will move through materials. Such insight is indispensable in sectors like HVAC (Heating, Ventilation, Air Conditioning), automotive cooling systems, and even in the culinary arts with the precise temperature control needed for certain cooking techniques.

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Most popular questions from this chapter

In natural convection mass transfer, the Grashof number is evaluated using density difference instead of temperature difference. Can the Grashof number evaluated this way be used in heat transfer calculations also?

Air flows in a 4-cm-diameter wet pipe at \(20^{\circ} \mathrm{C}\) and \(1 \mathrm{~atm}\) with an average velocity of \(4 \mathrm{~m} / \mathrm{s}\) in order to dry the surface. The Nusselt number in this case can be determined from \(\mathrm{Nu}=0.023 \mathrm{Re}^{0.8} \mathrm{Pr}^{0.4}\) where \(\mathrm{Re}=10,550\) and \(\operatorname{Pr}=0.731\). Also, the diffusion coefficient of water vapor in air is \(2.42 \times\) \(10^{-5} \mathrm{~m}^{2} / \mathrm{s}\). Using the analogy between heat and mass transfer, the mass transfer coefficient inside the pipe for fully developed flow becomes (a) \(0.0918 \mathrm{~m} / \mathrm{s}\) (b) \(0.0408 \mathrm{~m} / \mathrm{s}\) (c) \(0.0366 \mathrm{~m} / \mathrm{s}\) (d) \(0.0203 \mathrm{~m} / \mathrm{s}\) (e) \(0.0022 \mathrm{~m} / \mathrm{s}\)

Show that for an ideal gas mixture maintained at a constant temperature and pressure, the molar concentration \(C\) of the mixture remains constant but this is not necessarily the case for the density \(\rho\) of the mixture.

A researcher is using a 5 -cm-diameter Stefan tube to measure the mass diffusivity of chloroform in air at \(25^{\circ} \mathrm{C}\) and \(1 \mathrm{~atm}\). Initially, the liquid chloroform surface was \(7.00 \mathrm{~cm}\) from the top of the tube; and after 10 hours have elapsed, the liquid chloroform surface was \(7.44 \mathrm{~cm}\) from the top of the tube, which corresponds to \(222 \mathrm{~g}\) of chloroform being diffused. At \(25^{\circ} \mathrm{C}\), the chloroform vapor pressure is \(0.263 \mathrm{~atm}\), and the concentration of chloroform is zero at the top of the tube. If the molar mass of chloroform is \(119.39 \mathrm{~kg} / \mathrm{kmol}\), determine the mass diffusivity of chloroform in air.

A tank with a 2-cm-thick shell contains hydrogen gas at the atmospheric conditions of \(25^{\circ} \mathrm{C}\) and \(90 \mathrm{kPa}\). The charging valve of the tank has an internal diameter of \(3 \mathrm{~cm}\) and extends \(8 \mathrm{~cm}\) above the tank. If the lid of the tank is left open so that hydrogen and air can undergo equimolar counterdiffusion through the 10 -cm- long passageway, determine the mass flow rate of hydrogen lost to the atmosphere through the valve at the initial stages of the process.

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