At first, since the temperature is constant, for an ideal gas we have the following:
p1v1′=RT=p2v2′;v1′=v1/n;v2′=v2/nv1′v2′=p2p1
Then, we proceed to find the work for this type of process, where n* is the rate of gas that is being compressed on the device (n∗=12minkg×60s1min=0.2skg), and the relation between RT and p1v'1 to find:
W=∫pdv=∫(vn∗RT)dv=n∗RT∫vdvW=n∗RTlnv1′v2′=n∗p1v1′lnp2p1
Now, we proceed to substitute and we calculate the rate of work done as:
W=(0.2skg)(99kPa)(0.81kgm3)ln(600kPa99kPa)W=−28.8974skJ=−28.8974kW
Reference:
- Sears, F. W., & Zemansky, M. W. (1973). University physics.
Comments