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Pressure and Volume in an Adiabatic Process01:27

Pressure and Volume in an Adiabatic Process

Free expansion of a gas is an adiabatic process. However, there are few differences between free expansion and adiabatic expansion. During free expansion, no work is done, and there is no change in internal energy. But, for an adiabatic expansion, work is done, and there is a change in internal energy. During an adiabatic process, the relation between the pressure and volume is obtained from the condition for the adiabatic process, that is,
Efficiency of The Carnot Cycle01:16

Efficiency of The Carnot Cycle

The hypothetical Carnot cycle consists of an ideal gas subjected to two isothermal and two adiabatic processes. Since the internal energy of an ideal gas depends only on its temperature, which is the same before and after the completion of the Carnot cycle, there is no change in its internal energy. Hence, using the first law of thermodynamics, the total heat exchanged by the ideal gas equals the total work done. Thus, we can quantify the efficiency of the Carnot cycle via the heat exchanged...
Bioreactor Controls-II01:18

Bioreactor Controls-II

In aerobic fermentations, oxygen is vital for microbial growth and metabolite production. Since air comprises only about 20% oxygen and the gas is poorly soluble in water—just 9 ppm at 20°C—supplying sufficient oxygen becomes a critical challenge, especially in high-demand processes like yeast growth or citric acid production. Even a fully saturated broth may offer only a few seconds of oxygen availability.To address this, sterile or scrubbed air is introduced into the fermentor via a sparger...
Joule-Thomson Effect01:21

Joule-Thomson Effect

The Joule-Thomson effect, also known as the Joule-Kelvin effect, describes the temperature change of a fluid when it is forced through a valve or porous plug while keeping it in a thermally insulated environment. This experiment is called a throttling process. This is an important effect widely used in refrigeration and the liquefaction of gases.
This experiment forces high-pressure gas through a throttle valve or a porous plug to a lower-pressure region. The gas expands as it passes through to...
Adiabatic Processes for an Ideal Gas01:18

Adiabatic Processes for an Ideal Gas

When an ideal gas is compressed adiabatically, that is, without adding heat, work is done on it, and its temperature increases. In an adiabatic expansion, the gas does work, and its temperature drops. Adiabatic compressions actually occur in the cylinders of a car, where the compressions of the gas-air mixture take place so quickly that there is no time for the mixture to exchange heat with its environment. Nevertheless, because work is done on the mixture during the compression, its...
The Joule and Joule–Thomson Experiments01:23

The Joule and Joule–Thomson Experiments

Consider an adiabatic system composed of two chambers, A and B, designed such that no heat flows into or out of the system. Initially, chamber A is filled with a gas at a fixed temperature T1, pressure p1, and volume V1, while chamber B is evacuated. The gas is then gradually forced through a rigid, porous barrier to chamber B, ultimately reaching temperature T2, pressure p2, and volume V2. A piston on the right side maintains a constant pressure (p2), which is lower than p1. The significant...

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Related Experiment Video

Updated: Jul 16, 2026

Operation of a 25 KWth Calcium Looping Pilot-plant with High Oxygen Concentrations in the Calciner
06:34

Operation of a 25 KWth Calcium Looping Pilot-plant with High Oxygen Concentrations in the Calciner

Published on: October 25, 2017

Ventilation equations for improved exothermic process control.

John L McKernan1, Michael J Ellenbecker

  • 1National Institute for Occupational Safety and Health, Division of Surveillance Hazard Evaluation and Field Studies, Cincinnati, OH 45226, USA. jmckernan@cdc.gov

The Annals of Occupational Hygiene
|March 14, 2007
PubMed
Summary

New equations improve worker safety by accurately calculating airflow from exothermic processes, offering better ventilation control than older methods. This research addresses heat and contaminant exposure risks for millions of American workers.

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Thermal Preconditioning During Ex-vivo Lung Perfusion for the Rehabilitation of Damaged Lung Grafts before Transplantation
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Thermal Preconditioning During Ex-vivo Lung Perfusion for the Rehabilitation of Damaged Lung Grafts before Transplantation

Published on: October 31, 2025

Related Experiment Videos

Last Updated: Jul 16, 2026

Operation of a 25 KWth Calcium Looping Pilot-plant with High Oxygen Concentrations in the Calciner
06:34

Operation of a 25 KWth Calcium Looping Pilot-plant with High Oxygen Concentrations in the Calciner

Published on: October 25, 2017

Thermal Preconditioning During Ex-vivo Lung Perfusion for the Rehabilitation of Damaged Lung Grafts before Transplantation
09:34

Thermal Preconditioning During Ex-vivo Lung Perfusion for the Rehabilitation of Damaged Lung Grafts before Transplantation

Published on: October 31, 2025

Area of Science:

  • Occupational Health and Safety
  • Industrial Hygiene
  • Engineering Controls

Background:

  • Millions of American workers face risks from exothermic processes due to heat and contaminants.
  • Current engineering controls for exothermic processes are outdated, lacking improvements in heat transfer and meteorological theory.
  • No specific OSHA standard exists for heat exposure from exothermic processes, necessitating improved control techniques.

Purpose of the Study:

  • To develop and present new equations for calculating buoyant volumetric flow from exothermic processes.
  • To compare the proposed equations with existing models by Hemeon and ACGIH.
  • To enhance the design and efficiency of ventilation controls for exothermic processes.

Main Methods:

  • Reviewed physical properties, heat transfer, and meteorological theories of buoyant airflow.
  • Developed new equations for plume area, mean velocity, and flow.
  • Conducted numerical assessments and statistical analysis (ANOVA) to compare proposed equations with Hemeon and ACGIH models.

Main Results:

  • The proposed plume mean velocity equation yielded significantly higher means than ACGIH and Hemeon equations.
  • Proposed equations for plume area and flow showed significantly greater means than ACGIH and Hemeon at distances >1m.
  • The developed equations provide accurate solutions for total volumetric flow.

Conclusions:

  • The new equations offer improved accuracy for ventilation control design over existing methods.
  • Accurate volumetric flow data enables better hood design, placement, and sizing for worker protection.
  • This research provides critical parameters for optimizing ventilation efficacy and efficiency in exothermic processes.