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Dive into the research topics where Steven G. Penoncello is active.

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Featured researches published by Steven G. Penoncello.


Journal of Physical and Chemical Reference Data | 2000

Thermodynamic Properties of Air and Mixtures of Nitrogen, Argon, and Oxygen From 60 to 2000 K at Pressures to 2000 MPa

Eric W. Lemmon; R. T. Jacobsen; Steven G. Penoncello; Daniel G. Friend

A thermodynamic property formulation for standard dry air based upon available experimental p–ρ–T, heat capacity, speed of sound, and vapor–liquid equilibrium data is presented. This formulation is valid for liquid, vapor, and supercritical air at temperatures from the solidification point on the bubble-point curve (59.75 K) to 2000 K at pressures up to 2000 MPa. In the absence of reliable experimental data for air above 873 K and 70 MPa, air properties were predicted from nitrogen data in this region. These values were included in the determination of the formulation to extend the range of validity. Experimental shock tube measurements on air give an indication of the extrapolation behavior of the equation of state up to temperatures and pressures of 5000 K and 28 GPa. The available measurements of thermodynamic properties of air are summarized and analyzed. Separate ancillary equations for the calculation of dew and bubble-point pressures and densities of air are presented. In the range from the solidif...


Journal of Physical and Chemical Reference Data | 2009

Fundamental Equations of State for Parahydrogen, Normal Hydrogen, and Orthohydrogen

Jacob Leachman; R. T. Jacobsen; Steven G. Penoncello; Eric W. Lemmon

If the potential for a boom in the global hydrogen economy is realized, there will be an increase in the need for accurate hydrogen thermodynamic property standards. Based on current and anticipated needs, new fundamental equations of state for parahydrogen, normal hydrogen, and orthohydrogen were developed to replace the existing property models. To accurately predict thermophysical properties near the critical region and in liquid states, the quantum law of corresponding states was applied to improve the normal hydrogen and orthohydrogen formulations in the absence of available experimental data. All three equations of state have the same maximum pressure of 2000MPa and upper temperature limit of 1000K. Uncertainty estimates in this paper can be considered to be estimates of a combined expanded uncertainty with a coverage factor of 2 for primary data sets. The uncertainty in density is 0.04% in the region between 250 and 450K and at pressures up to 300MPa. The uncertainties of vapor pressures and satura...


International Journal of Thermophysics | 2004

A Fundamental Equation for Calculation of the Thermodynamic Properties of Ethanol

Heather Dillon; Steven G. Penoncello

A formulation for the thermodynamic properties of ethanol (C2H5OH) in the liquid, vapor, and saturation states is presented. The formulation is valid for single-phase and saturation states from 250 to 650 K at pressures up to 280 MPa. The formulation includes a fundamental equation and ancillary functions for the estimation of saturation properties. The experimental data used to determine the fundamental equation include pressure-density-temperature, ideal gas heat capacity, speed of sound, and vapor pressure. Saturation values computed from the ancillary functions were used to ensure thermodynamic consistency at the vapor-liquid phase boundary. Comparisons between experimental data and values computed using the fundamental equation are given to verify the uncertainties in the calculated properties. The formulation presented may be used to compute densities to within ±0.2%, heat capacities to within ±3%, and speed of sound to within ±1%. Saturation values of the vapor pressure and saturation densities are represented to within ±0.5%, except near the critical point.


Experimental Thermodynamics | 2000

18 Multiparameter equations of state

R. T. Jacobsen; Steven G. Penoncello; Eric W. Lemmon; Roland Span

Publisher Summary Accurate thermophysical properties of fluids are needed for the development of reliable mathematical models of energy systems. Although significant improvements are being made in predicting thermodynamic properties of pure fluids and mixtures using theory-based methods, there is a need for more accurate equations of state both for applications in engineering system design and analysis and to satisfy scientific data needs. Current practice in the development of computer programs, property tables, and charts involves the correlation of selected experimental data for a particular fluid or mixture using a model, which is accurate for calculating properties over a wide range of pressures and temperatures. A typical thermodynamic property formulation is based on an equation of state, which allows the correlation and computation of all thermodynamic properties of the fluid, including properties such as entropy that cannot be measured directly. The term “fundamental equation” is often used in the literature to refer to empirical descriptions of one of four fundamental relations: internal energy as a function of volume and entropy, enthalpy as a function of pressure and entropy, Gibbs energy as a function of pressure and temperature, and Helmholtz energy as a function of density and temperature. Modern equations of state for pure fluid properties are usually fundamental equations explicit in the Helmholtz energy as a function of density and temperature.


International Journal of Thermophysics | 1995

A thermodynamic property formulation for cyclohexane

Steven G. Penoncello; R. T. Jacobsen; A. R. H. Goodwin

A formulation for the thermodynamic properties of cyclohexane is presented. The equation is valid for single-phase and saturation states from the melting line to 700 K at pressures up to 80 MPa. It includes a fundamental equation explicit in reduced Helmholtz energy with independent variables of reduced density and temperature. The functional form and coefficients of the ancillary equations were determined by weighted linear regression analyses of evaluated experimental data. An adaptive regression algorithm was used to determine the final equation. To ensure correct thermodynamic behavior of the Helmholtz energy surface the coefficients of the fundamental equation were determined with multiproperty fitting, Pressure-density-temperature (P-p-T) and isobaric heat capacity (Cp-P-T) data were used to develop the fundamental equation, SaturationP-p-T values, calculated from the estimating functions, were used to ensure thermodynamic consistency at the vapor-liquid phase boundary. Separate functions were used for the vapor pressure, saturated liquid density, saturated vapor density. ideal-gas heat capacity. and pressure on the melting curve, Comparisons between experimental data and values calculated using the fundamental equation are given to verify the accuracy of the formulation. The formulation given here may be used to calculate densities within ±0.1 %, heat capacities to within ±2 %. and speed of sound to within ± 1 %, except near the critical point.


Journal of Physical and Chemical Reference Data | 2003

A Fundamental Equation for Trifluoromethane (R-23)

Steven G. Penoncello; Eric W. Lemmon; R. T. Jacobsen; Zhengjun Shan

A new formulation for the thermodynamic properties of trifluoromethane (R-23) is presented. The formulation is valid for single-phase and saturation states for temperatures from the triple point (118.02 K) to 475 K, pressures up to 120 MPa, and densities up to 24.31 mol/dm3. The formulation includes a fundamental equation and ancillary functions for the estimation of saturation properties. The experimental data used to determine the fundamental equation included pressure–density–temperature (p–ρ–T), isobaric heat capacity (cp–p–T), isochoric heat capacity (cν–ρ–T), saturation heat capacity (cσ), speed of sound (w–p–T), and vapor pressure. A nonlinear regression algorithm was used to determine the constants and exponents of various functions within the formulation. Experimental data and values computed using the formulation are compared to verify the uncertainties in the calculated properties. The formulation presented may be used to compute densities to within ±0.1%, heat capacities to within ±0.5%, speed...


Fluid Phase Equilibria | 1992

A thermodynamic property formulation for air

R. T. Jacobsen; Steven G. Penoncello; Steven Beyerlein; W. P. Clarke; Eric W. Lemmon

Abstract A thermodynamic property formulation for air based upon new experimental P-ϱ-T, isochoric heat capacity and velocity of sound data has been developed. This model treats air as a pseudo-pure fluid for a wide-range of temperatures and pressures and provides for calculation of energy, heat capacity, entropy and velocity of sound in addition to pressure, density and temperature. This new formulation is valid for temperatures from 60 to 873 K at pressures to 70 MPa and is based on new measurements of the properties of liquid air recently completed at the National Institute of Standards and Technology (NIST) in Boulder, Colorado. The accuracies of properties calculated using the new thermodynamic property formulation are established by comparison to available experimental data.


Journal of Physical and Chemical Reference Data | 2014

An Equation of State for the Thermodynamic Properties of Cyclohexane

Yong Zhou; Jun Liu; Steven G. Penoncello; Eric W. Lemmon

An equation of state for cyclohexane has been developed using the Helmholtz energy as the fundamental property with independent variables of density and temperature. Multi-property fitting technology was used to fit the equation of state to data for pρT, heat capacities, sound speeds, virial coefficients, vapor pressures, and saturated densities. The equation of state was developed to conform to the Maxwell criteria for two-phase vapor-liquid equilibrium states, and is valid from the triple-point temperature to 700 K, with pressures up to 250 MPa and densities up to 10.3 mol dm−3. In general, the uncertainties (k = 2, indicating a level of confidence of 95%) in density for the equation of state are 0.1% (liquid and vapor) up to 500 K, and 0.2% above 500 K, with higher uncertainties within the critical region. Between 283 and 473 K with pressures lower than 30 MPa, the uncertainty is as low as 0.03% in density in the liquid phase. The uncertainties in the speed of sound are 0.2% between 283 and 323 K in th...


Journal of Supercritical Fluids | 1995

Isobaric heat capacities of carbon dioxide and argon between 323 and 423 K and at pressures up to 25 MPa

Laurent Dordain; Jean-Yves Coxam; Jacques R. Quint; Jean-Pierre E. Grolier; Eric W. Lemmon; Steven G. Penoncello

Abstract The isobaric specific heat capacities cp of carbon dioxide and argon have been measured between 323 and 423 K at pressures up to 25 MPa. The present results obtained by means of the experimental technique recently designed for gases1 are compared with literature data and with values calculated from different equations of state.


International Journal of Thermophysics | 1994

An extended corresponding-states model for predicting thermodynamic properties of N2-Ar-O2 mixtures including vapor-liquid equilibrium

W. P. Clarke; R. T. Jacobsen; Eric W. Lemmon; Steven G. Penoncello; Steven Beyerlein

A formulation developed previously for the prediction of the thermodynamic properties of single-phase states of binary and ternary mixtures in the nitrogen-argon-oxygen system has been revised to include the calculation of vapor-liquid equilibrium (VLE) properties. The model is based on the theory of extended corresponding states with van der Waals mixing rules. Binary interaction parameters have been determined with single-phaseP-p-T and vaporliquid equilibrium data to improve the accuracy of thermodynamic property predictions. The model accurately represents single-phase and vapor-liquid equilibrium properties over a wide range of compositions for binary and ternary mixtures. Comparisons of calculated properties to selected mixture data for both single-phase and VLE states are included.

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Eric W. Lemmon

National Institute of Standards and Technology

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Jacob Leachman

Washington State University

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Daniel G. Friend

National Institute of Standards and Technology

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