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What is the modified latent heat of vaporization? For what is it used? How does it differ from the ordinary latent heat of vaporization?

Short Answer

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Answer: The main difference between the modified latent heat of vaporization and the ordinary latent heat of vaporization lies in the inclusion of sensible heat. Modified latent heat factors in the energy required to raise the temperature of a substance to its boiling point in addition to the energy required for phase change, while the ordinary latent heat strictly refers to the energy needed to undergo a phase change from liquid to vapor state at the boiling point, without considering the temperature change.

Step by step solution

01

Understanding Latent Heat of Vaporization

The latent heat of vaporization is the amount of heat required to convert a given mass of liquid at its boiling point to a vapor without changing its temperature. It is used to describe and quantify the energy needed in phase changes involving a substance's transition between the liquid and vapor states.
02

Introducing Modified Latent Heat of Vaporization

The modified latent heat of vaporization refers to the amount of heat required to transform a liquid into a vapor when the temperature of the liquid is below its boiling point. In this case, an added component of sensible heat is considered, which is the heat needed to bring the substance to its boiling point before the phase transition occurs. In other words, modified latent heat encompasses both sensible heat (raising the temperature) and actual latent heat (phase change).
03

Usage of Modified Latent Heat of Vaporization

Modified latent heat of vaporization is used in various applications like power generation, refrigeration, and air conditioning systems. It is particularly helpful in understanding and designing systems that operate below boiling points or those that work with a combination of phase changes and temperature changes. The consideration of modified latent heat allows engineers and scientists to accurately calculate heat exchange and energy requirements for various scenarios where the temperature of the liquid is below the boiling point.
04

Difference between Ordinary Latent Heat and Modified Latent Heat of Vaporization

The primary difference between the ordinary latent heat and the modified latent heat of vaporization lies in the inclusion of sensible heat. The ordinary latent heat of vaporization strictly refers to the energy needed to undergo a phase change from liquid to vapor state at the boiling point, without considering the temperature change. Conversely, modified latent heat factors in the energy required to raise the temperature of a substance to its boiling point in addition to the energy required for phase change.

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Most popular questions from this chapter

Steam condenses at \(50^{\circ} \mathrm{C}\) on the tube bank consisting of 20 tubes arranged in a rectangular array of 4 tubes high and 5 tubes wide. Each tube has a diameter of \(3 \mathrm{~cm}\) and a length of \(5 \mathrm{~m}\), and the outer surfaces of the tubes are maintained at \(30^{\circ} \mathrm{C}\). The rate of condensation of steam is (a) \(0.12 \mathrm{~kg} / \mathrm{s}\) (b) \(0.28 \mathrm{~kg} / \mathrm{s}\) (c) \(0.31 \mathrm{~kg} / \mathrm{s}\) (d) \(0.45 \mathrm{~kg} / \mathrm{s}\) (e) \(0.62 \mathrm{~kg} / \mathrm{s}\) (For water, use $\rho_{l}=992.1 \mathrm{~kg} / \mathrm{m}^{3}, \mu_{l}=0.653 \times 10^{-3} \mathrm{~kg} / \mathrm{m} \cdot \mathrm{s}\(, \)\left.k_{t}=0.631 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}, c_{p l}=4179 \mathrm{~J} / \mathrm{kg} \cdot{ }^{\circ} \mathrm{C}, h_{f g} \oplus T_{\omega}=2383 \mathrm{~kJ} / \mathrm{kg}\right)$

A 1 -mm-diameter long electrical wire submerged in water at atmospheric pressure is dissipating \(4100 \mathrm{~W} / \mathrm{m}\) of heat, and the surface temperature reaches \(128^{\circ} \mathrm{C}\). If the experimental constant that depends on the fluid is \(n=1\), determine the nucleate boiling heat transfer coefficient and the value of the experimental constant $C_{\text {sf. }}$.

Saturated ammonia vapor at \(25^{\circ} \mathrm{C}\) condenses on the outside surface of 16 thin-walled tubes, \(2.5 \mathrm{~cm}\) in diameter, arranged horizontally in a \(4 \times 4\) square array. Cooling water enters the tubes at \(14^{\circ} \mathrm{C}\) at an average velocity of \(2 \mathrm{~m} / \mathrm{s}\) and exits at \(17^{\circ} \mathrm{C}\). Calculate \((a)\) the rate of \(\mathrm{NH}_{3}\) condensation, (b) the overall heat transfer coefficient, and \((c)\) the tube length.

In condensate flow, how is the wetted perimeter defined? How does wetted perimeter differ from ordinary perimeter?

A 1-mm-diameter nickel wire with electrical resistance of $0.129 \Omega / \mathrm{m}$ is submerged horizontally in water at atmospheric pressure. Determine the electrical current at which the wire would be in danger of burnout in nucleate boiling.

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