Thermodynamics, Heat Motors And Refrigerating Machines
Thermodynamics, Heat Motors And Refrigerating Machines
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(814) For the same cnt-oflf, the isothermal will lie wholly above the adiabatic, and U^ in equation (314) will exceed U in equation (306). In order to secure isothermal expansion it is necessary to heat the air in the cylinder during expan- sion. It is not, however, practical to maintain a uniform temperature in this way. The very low final temperature has, however, in practice been prevented by working the air in one cylinder through a part of the full range of pressures, then exhausting into ...a receiver and there heating it, after which it is worked in a second cylinder.
{e) Expansion isothermal a/nd complete. In this case the terminal pressure H (7, Fig. 72, will equal the back pressure H E\ or j?, = p^ in equation (314) ; • •. U^DABC^ OBOE = jp, v^ log^ r = 122.5 t, log^^ r. (315) Weight of air per minute. Let W be the number of pounds of working air necessary to deliver N horse-powers per minute, then, since U is the work in foot-pounds per pound of air, W U^ 33000 iT; ...Tr=??^.
What to read after Thermodynamics, Heat Motors And Refrigerating Machines?
You can find similar books in the "Read Also" column, or choose other free books by De Volson Wood to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
(814) For the same cnt-oflf, the isothermal will lie wholly above the adiabatic, and U^ in equation (314) will exceed U in equation (306). In order to secure isothermal expansion it is necessary to heat the air in the cylinder during expan- sion. It is not, however, practical to maintain a uniform temperature in this way. The very low final temperature has, however, in practice been prevented by working the air in one cylinder through a part of the full range of pressures, then exhausting into ...a receiver and there heating it, after which it is worked in a second cylinder.
{e) Expansion isothermal a/nd complete. In this case the terminal pressure H (7, Fig. 72, will equal the back pressure H E\ or j?, = p^ in equation (314) ; • •. U^DABC^ OBOE = jp, v^ log^ r = 122.5 t, log^^ r. (315) Weight of air per minute. Let W be the number of pounds of working air necessary to deliver N horse-powers per minute, then, since U is the work in foot-pounds per pound of air, W U^ 33000 iT; ...Tr=??^.
What to read after Thermodynamics, Heat Motors And Refrigerating Machines?
You can find similar books in the "Read Also" column, or choose other free books by De Volson Wood to read onlineMoreLess
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