Elementary Treatise On Physics Experimental And
Elementary Treatise On Physics Experimental And
The book Elementary Treatise On Physics Experimental And was written by author Here you can read free online of Elementary Treatise On Physics Experimental And book, rate and share your impressions in comments. If you don't know what to write, just answer the question: Why is Elementary Treatise On Physics Experimental And a good or bad book?
Where can I read Elementary Treatise On Physics Experimental And for free?
In our eReader you can find the full English version of the book. Read Elementary Treatise On Physics Experimental And Online - link to read the book on full screen. Our eReader also allows you to upload and read Pdf, Txt, ePub and fb2 books. In the Mini eReder on the page below you can quickly view all pages of the book - Read Book Elementary Treatise On Physics Experimental And
In our eReader you can find the full English version of the book. Read Elementary Treatise On Physics Experimental And Online - link to read the book on full screen. Our eReader also allows you to upload and read Pdf, Txt, ePub and fb2 books. In the Mini eReder on the page below you can quickly view all pages of the book - Read Book Elementary Treatise On Physics Experimental And
What reading level is Elementary Treatise On Physics Experimental And book?
To quickly assess the difficulty of the text, read a short excerpt:
It is to be observed that, at the commencement of the experiment, the condensed vapour passes out at the temperature /, while at the conclusion its temperature is ; we may, however, assume that its mean temperature . , f\ during the experiment is . The vapour M after condensation has therefore parted with a quantity of heat M(T V, while the heat disengaged in liquefaction is represented by M*. The quantity of heat absorbed by the cold water, the worm, and the vessel is m(B-t). Hence from which ...x is obtained. Despretz found that the latent heat of steam at 100 is 540 ; that is, a pound of water at 100 absorbs, in vaporising, as much heat as would raise 540 pounds of water through i. The values for the latent heat of aqueous vapour obtained by Regnault at temperatures between 65 and 100, and more recently by Dieterici at o, and by E. H. Griffiths at intermediate temperatures, are represented with great accuracy by the formula L = 59673 -o6oi/. Thus, at 100, L = 536-63.
Berthelot used the apparatus represented in fig.
What to read after Elementary Treatise On Physics Experimental And?
You can find similar books in the "Read Also" column, or choose other free books by A Adolphe Ganot to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
It is to be observed that, at the commencement of the experiment, the condensed vapour passes out at the temperature /, while at the conclusion its temperature is ; we may, however, assume that its mean temperature . , f\ during the experiment is . The vapour M after condensation has therefore parted with a quantity of heat M(T V, while the heat disengaged in liquefaction is represented by M*. The quantity of heat absorbed by the cold water, the worm, and the vessel is m(B-t). Hence from which ...x is obtained. Despretz found that the latent heat of steam at 100 is 540 ; that is, a pound of water at 100 absorbs, in vaporising, as much heat as would raise 540 pounds of water through i. The values for the latent heat of aqueous vapour obtained by Regnault at temperatures between 65 and 100, and more recently by Dieterici at o, and by E. H. Griffiths at intermediate temperatures, are represented with great accuracy by the formula L = 59673 -o6oi/. Thus, at 100, L = 536-63.
Berthelot used the apparatus represented in fig.
What to read after Elementary Treatise On Physics Experimental And?
You can find similar books in the "Read Also" column, or choose other free books by A Adolphe Ganot to read onlineMoreLess
Write Review:
User Reviews: