A Treatise On the Compound Steam Engine, in Two Parts. Pt. I
A Treatise On the Compound Steam Engine, in Two Parts. Pt. I
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In our eReader you can find the full English version of the book. Read A Treatise On the Compound Steam Engine, in Two Parts. Pt. I 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 A Treatise On the Compound Steam Engine, in Two Parts. Pt. I
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we have V, _ V, being the volume of the high cylinder, and to be so regarded in every applica- tion. Hence V,' in the present case is to replace V x of Eq. (10) or (11). Our ex- pression for the whole work of engine t per stroke is, therefore, pv* / i \ JJ =-7~ 1 - A Ti 7fl — ^-r)- p 3 Y * • • ( 12 ) rjjn — 1)\ r m-\j 32 v / r 1 being the ratio of expansion in the Digitized by GoOgle 117 high-pressure cylinder itself, and r the ratio of the entire expansion C to G, also P,=the boiler pressure (...absolute), Y 1 the volume AE of high-pressure, and V 2 the volume AF of the low-pressure cylinder.
The work performed in the low-press- ure cylinder alone, according to (6), is AF AHDGFA-P 3 V 8 =EDGFE Jt-P.V, EF A ExED j 1 >AF m-1 j* / AF y^EF" \AE/ -P.V.
The work performed in the high-press- ure cylinder is, of course, the difference between the last equation and (12).
For the case x=1, we have U=^(l+hyp.log.r)-P s V 5 and the work performed in the low-press- ure cylinder according to (8) is AF AF ^AExED^-hyp.log.^ VP V V -1r vT-V h ^- **• v: d by Google 118 II.
What to read after A Treatise On the Compound Steam Engine, in Two Parts. Pt. I?
You can find similar books in the "Read Also" column, or choose other free books by S W Stillman Williams Robinson to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
we have V, _ V, being the volume of the high cylinder, and to be so regarded in every applica- tion. Hence V,' in the present case is to replace V x of Eq. (10) or (11). Our ex- pression for the whole work of engine t per stroke is, therefore, pv* / i \ JJ =-7~ 1 - A Ti 7fl — ^-r)- p 3 Y * • • ( 12 ) rjjn — 1)\ r m-\j 32 v / r 1 being the ratio of expansion in the Digitized by GoOgle 117 high-pressure cylinder itself, and r the ratio of the entire expansion C to G, also P,=the boiler pressure (...absolute), Y 1 the volume AE of high-pressure, and V 2 the volume AF of the low-pressure cylinder.
The work performed in the low-press- ure cylinder alone, according to (6), is AF AHDGFA-P 3 V 8 =EDGFE Jt-P.V, EF A ExED j 1 >AF m-1 j* / AF y^EF" \AE/ -P.V.
The work performed in the high-press- ure cylinder is, of course, the difference between the last equation and (12).
For the case x=1, we have U=^(l+hyp.log.r)-P s V 5 and the work performed in the low-press- ure cylinder according to (8) is AF AF ^AExED^-hyp.log.^ VP V V -1r vT-V h ^- **• v: d by Google 118 II.
What to read after A Treatise On the Compound Steam Engine, in Two Parts. Pt. I?
You can find similar books in the "Read Also" column, or choose other free books by S W Stillman Williams Robinson to read onlineMoreLess
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