Biochemical Research 1912 13
Biochemical Research 1912 13
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525 size in liquid and vapor, or do not in other ways gain energy. 1 I believe the internal latent heat of vaporization consists of at least three parts, not two as is often stated, these three parts are : (i) the heat consumed in expanding against external pressure, or E; (2), the heat consumed in overcoming molec- ular cohesion, or A; (3), heat consumed in increasing internal molecular potential energy by expanding the molecule, or increasing its energy of rotation, or I. This last factor is ...often overlooked. If L is the total latent heat of vaporiza- tion the expression should be : L E I == A. And if mole- cules attract inversely as the square of the distance we should have (I, E I)/(V^ VDJ - /.
There are two principal reasons why it cannot be assumed that all the internal latent heat of vaporization goes to in- creasing the potential energy by separating the molecules against the force of their molecular cohesions. The first of these reasons is that the value "b, " of van der Waals' equa- tion, has to be taken larger in the vapor than in the liquid for some distance below the critical point.
What to read after Biochemical Research 1912 13?
You can find similar books in the "Read Also" column, or choose other free books by University of Chicago Biochemical Laboratory to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
525 size in liquid and vapor, or do not in other ways gain energy. 1 I believe the internal latent heat of vaporization consists of at least three parts, not two as is often stated, these three parts are : (i) the heat consumed in expanding against external pressure, or E; (2), the heat consumed in overcoming molec- ular cohesion, or A; (3), heat consumed in increasing internal molecular potential energy by expanding the molecule, or increasing its energy of rotation, or I. This last factor is ...often overlooked. If L is the total latent heat of vaporiza- tion the expression should be : L E I == A. And if mole- cules attract inversely as the square of the distance we should have (I, E I)/(V^ VDJ - /.
There are two principal reasons why it cannot be assumed that all the internal latent heat of vaporization goes to in- creasing the potential energy by separating the molecules against the force of their molecular cohesions. The first of these reasons is that the value "b, " of van der Waals' equa- tion, has to be taken larger in the vapor than in the liquid for some distance below the critical point.
What to read after Biochemical Research 1912 13?
You can find similar books in the "Read Also" column, or choose other free books by University of Chicago Biochemical Laboratory to read onlineMoreLess
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