Thermodynamics - Work done per unit mass

In summary: As for density, it depends on the equation you use for air. Some equations use density, others use specific volume. But in any case, the gas constant will be there.
  • #1
davcrai
13
0

Homework Statement



A sample of dry air has initial pressure p1 = 1000 hPa and temperature T1 = 300k. It undergoes a process that takes it to a new pressure p2 = 500 hPa with unchanged temperature T2 = T1. Compute the mechanical work per unit mass performed by the sample under the following scenarios:
a) Isochoric pressure reduction to p2 followed by isobaric expansion to final state.
b) Isobaric expansion to final specific volume s2 followed by isochoric pressure reduction to final state.
c) Isothermal expansion to final state.

Homework Equations



work = ∫pds
s = Volume/mass

The Attempt at a Solution



a) I think pressure held constant at 500 and the integral preformed between s1 and s2, to get -500*(s2-s1).

b) The integral is ∫p(s)ds with limits s1 to s2 from to give p(s)*(s2-s1), then evaluate at p = 500 for the same result ?

c) The previous two were isothermal?
 
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  • #2


davcrai said:

Homework Statement



A sample of dry air has initial pressure p1 = 1000 hPa and temperature T1 = 300k. It undergoes a process that takes it to a new pressure p2 = 500 hPa with unchanged temperature T2 = T1. Compute the mechanical work per unit mass performed by the sample under the following scenarios:
a) Isochoric pressure reduction to p2 followed by isobaric expansion to final state.
b) Isobaric expansion to final specific volume s2 followed by isochoric pressure reduction to final state.
c) Isothermal expansion to final state.

Homework Equations



work = ∫pds
s = Volume/mass

The Attempt at a Solution



a) I think pressure held constant at 500 and the integral preformed between s1 and s2, to get -500*(s2-s1).
Looks reasonable so far, but you need to figure out values for s1 and s2. Also, watch the units.

b) The integral is ∫p(s)ds with limits s1 to s2 from to give p(s)*(s2-s1), then evaluate at p = 500 for the same result ?
The pressure is not 500 hPa for this one; the first step is isobaric in this case. Try drawing yourself a PV diagram, to help figure out what is going on.

c) The previous two were isothermal?
Um, no, they were not. There were two steps, one isochoric and one isobaric. So the temperature changed during processes (a) and (b), even though it ended up at the initial temperature.

This time, it is isothermal during the entire process.
 
  • #3


ok, so I think for the second one you hold p constant at 1000hPa for the integration then evaluate between s1 and s2?
Still unsure about the third one?
 
  • #4


davcrai said:
ok, so I think for the second one you hold p constant at 1000hPa for the integration then evaluate between s1 and s2?
Yes. You'll also need to figure out what s1 and s2 are.
Still unsure about the third one?
You need to find an equation that relates P and s, using the fact that T=constant. (Hint: the substance is air, and air is a gas.)

Once you have the relation between P and s, do the integral ∫p·ds.
 
  • #5


Hmmm, might it include density and a gas constant by any chance...
Thanks
 
  • #6


It would definitely include the gas constant.
 

FAQ: Thermodynamics - Work done per unit mass

What is thermodynamics?

Thermodynamics is a branch of physics that deals with the relationships between heat, energy, and work. It studies how these factors interact and how they affect the properties of matter.

What is work done per unit mass?

Work done per unit mass is a thermodynamic quantity that measures the amount of work that is done on or by a material per unit mass. It is often denoted as W/m and is measured in units of joules per kilogram (J/kg).

How is work done per unit mass calculated?

Work done per unit mass can be calculated using the equation W/m = ΔU + ΔKE + ΔPE, where ΔU is the change in internal energy, ΔKE is the change in kinetic energy, and ΔPE is the change in potential energy. This equation is based on the first law of thermodynamics, which states that the change in internal energy of a system is equal to the heat added to the system minus the work done by the system.

What is the significance of work done per unit mass in thermodynamics?

Work done per unit mass is an important concept in thermodynamics because it helps us understand how energy is transferred and transformed within a system. It also allows us to quantify the amount of work that is required to change the state of a material.

How does work done per unit mass relate to other thermodynamic quantities?

Work done per unit mass is closely related to other thermodynamic quantities, such as heat, internal energy, and enthalpy. It is also related to the laws of thermodynamics, which govern the behavior of energy in a system. Understanding how work done per unit mass relates to these other quantities is essential in studying and analyzing thermodynamic processes.

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