The classical rule, recognized by Kelvin, is that the pressure exerted by the calorimetric material is fully and rapidly determined solely by its temperature and volume; this rule is for changes that do not involve phase change, such as melting of ice.
32.
For measurements at experimentally controlled temperature, it is again assumed that the volume V \ of the body of calorimetric material can be expressed as a function V ( T, p ) \ of its temperature T \ and pressure p \, with the same provisos as mentioned just above.
33.
When a small increment of heat is gained by a calorimetric body, with small increments, \ delta V \ of its volume, and \ delta T \ of its temperature, the increment of heat, \ delta Q \, gained by the body of calorimetric material, is given by
34.
When a small increment of heat is gained by a calorimetric body, with small increments, \ delta V \ of its volume, and \ delta T \ of its temperature, the increment of heat, \ delta Q \, gained by the body of calorimetric material, is given by
35.
As the topic of cold fusion gains a more sound experimental footing, divorced from absurd open system calorimetric measurements, and focused on direct measurement of high energy particles generated in reproducible experimental apparatus, perhaps it is time that a higher class of editor take over deciding what research is appropriate to include.
36.
In 1932, Frederick Rossini, Edward W . Washburn, and Mikkel Frandsen authored The Calorimetric Determination of the Intrinsic Energy of Gases as a Function of the Pressure . This experiment resulted in the development of the Washburn Correction for bomb calorimetry, a decrease or correction of the results of a calorimetric procedure to normal states.
37.
In 1932, Frederick Rossini, Edward W . Washburn, and Mikkel Frandsen authored The Calorimetric Determination of the Intrinsic Energy of Gases as a Function of the Pressure . This experiment resulted in the development of the Washburn Correction for bomb calorimetry, a decrease or correction of the results of a calorimetric procedure to normal states.
38.
Based on the examination of published reports, reprints, numerous communications to the Panel and several site visits, the Panel concludes that the experimental results of excess heat from calorimetric cells reported to date do not present convincing evidence that useful sources of energy will result from the phenomena attributed to cold fusion . . . . The Panel concludes that the experiments reported to date do not present convincing evidence to associate the reported anomalous heat with a nuclear process . . ..
39.
For a time-dependent process of heating of the calorimetric material, defined by a continuous joint progression P ( t _ 1, t _ 2 ) \ of V ( t ) \ and T ( t ) \, starting at time t _ 1 \ and ending at time t _ 2 \, there can be calculated an accumulated quantity of heat delivered, \ Delta Q ( P ( t _ 1, t _ 2 ) ) \,.
40.
Other methods have been used historically, such as volumetric and calorimetric methods, as I'm sure the authors know . ( 5 ) More history of the concept would be good . ( 6 ) I appreciate the need for summary style to keep Featured Articles short, but the applications section seems rushed and random . ( 7 ) At the risk of adding yet another random example, chelation changes due to titrations might fit there nicely, with picturesque applications ranging from soils and plants ( why do blueberries grow in acidic soil ? ) to modern biochemistry ( elution of His tags from Ni columns, metal-ion binding in proteins and nucleic acids ).
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