Work: Difference between revisions
Jump to navigation
Jump to search
Carl McBride (talk | contribs) No edit summary |
(W=-pdV on compression or expansion, but always ''upon'' (I am 98% sure)) |
||
Line 1: | Line 1: | ||
The mechanical '''work''', ''W'', performed | The mechanical '''work''', ''W'', performed ''upon'' a gas is given by | ||
:<math>W = - \int_\alpha^\beta p ~dV</math> | :<math>W = - \int_\alpha^\beta p ~dV</math> | ||
where <math>\alpha</math> and <math>\beta</math> are points in state space, ''p'' is the [[pressure]] | where <math>\alpha</math> and <math>\beta</math> are points in state space, ''p'' is the [[pressure]] | ||
and ''V'' is the volume. | and ''V'' is the volume. The mechanical work done ''by'' the gas has the opposite sign (a common | ||
source of mistakes). | |||
For reversible changes | For reversible changes, | ||
:<math>\left.dW\right.=-p~dV </math> | :<math>\left.dW\right.=-p~dV </math> |
Revision as of 10:07, 8 June 2009
The mechanical work, W, performed upon a gas is given by
where and are points in state space, p is the pressure and V is the volume. The mechanical work done by the gas has the opposite sign (a common source of mistakes).
For reversible changes,
and for irreversible changes