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Thermodynamic Problem

awibroe
14-Alexandrite

Thermodynamic Problem

Hello to all,

 

I am having another 'simple' moment where I am going round in circles and am starting to feel a bit dim.

 

In the attached is a simple thermo question I am trying to complete.

 

I have completed a-c with some ease but am struggling with d. where the hint is to evaluate the integral of pressure over dVolume in the associated Pressure/Volume graph. 

 

I know that the integral of an isothermal expansion is either P*V*In(r) = heat supplied or m*R*T*In(r)

 

Where P and V are the initial (Pre-expansion) Pressure and Volume respectively and r is the ratio of expansion i.e. V2/V1. m being mass and R being the gass constant. 

 

As all figures given are specific i.e. no mass of air is specified I don't beleive I can use mRTIn(r) but cannot evaluate PVIn(r) as I don't know what the initial volume is...

 

I know that the heat supplied (well my calculations beleive it is) 187.5 kJ/kg. 

 

I beleive the approach is to calculate the volumes from the integral and then with this to find the pressure noting PV/T = Constant. 

 

Any help, as always, really appreciated.

 

Andy

16 REPLIES 16
awibroe
14-Alexandrite
(To:awibroe)

Sorry I should have added:

 

P1 = 800 kN/m^2

T1 = 750 K

R = 0.287kJ/kgK

awibroe
14-Alexandrite
(To:awibroe)

And I am obviously trying to find P2 and to do that beleive I need V1 and V2.

awibroe
14-Alexandrite
(To:awibroe)

So after some further thought, I have an approach but would appreciate someone wiser than I validating this approach...

 

Noting that I have the heat input to the isothermal expansion which is in kJ/kg I have negated m (kg) from the integral mRTIn(r) which would give a result in kJ/kg which is what I am after.

 

Then I can manipulate RTIn(r) to isolate In(r). Then by evaluating e to the power of the result of In(r) should give me r i.e. the expansion ratio i.e. V2/V1. This should then be an identity with P1/P2 noting P1*P2 = V1*V2 and I can then isolate P2 noting I have P1.

 

Any thoughts?

 

A

LucMeekes
23-Emerald III
(To:awibroe)

How about a Mathcad sheet...?

awibroe
14-Alexandrite
(To:LucMeekes)

Luc,

 

Yeah Sorry that would be logical. I have been without MC today and working by hand would you beleive. I should be up and running electronicly tomorrow.

 

A

 

 

Ok, let's see the "by hand"

awibroe
14-Alexandrite
(To:Fred_Kohlhepp)

Fred,

 

Definately is 'Homework'.

 

I am not about cheating, I am all about learning as you hopefully know by now.

 

So where I have got to:

 

I have crudly sketched a PV and a TS diagram and have calauated as follows.

 

Known values:

 

R= 0.287kJ/kgK  

Change in Entropy (in Expansion which should also be the same for Contraction)

Delta s = 0.25 kJ/kg

Net Work W = 100 kJ/kg

Aboslute Temperature at point 1 on a PV diagram i.e. before isothermal expansion = 750 K

Pressure at point 1 = 800 kN/m^2

 

My first step was to find the lower temperature and amount of heat rejected during isothemal compression. I note that the area of the square created in a TS graph will equal the net work. i.e. the product of change in entropy and change in temperature will be the net work. Therefore dividing the net work by the change in entropy should give the change in Temperature i.e.

 

Delta T = W/Delta s = 100 kJ/kg / 0.25 kJ/kgK = 400 K.

 

Ergo T2 i.e. lower Temperature = T1 - Delta T = 750K - 400K = 350K 

 

Next I note that the heat rejected by the cycle in isothermal compression is equal to the product of the Temperature (T4) after compression the change in entropy. i.e.

 

Qc = T4*Delta s = 350K*0.25kJ/kgK = 87.5 kj/kg

 

To verify this I looked at the heat taken in during isothermal expansion as Qh = T1*Delta s = 750K*0.25kJ/kgK = 187.5kJ.

 

This holds true with the first law i.e. Sum of Q = Sum of W noting heat in is positive and heat out is negative 

 

187.5 + (-87.5) = 100 

 

Then the thermal Efficiency being T1-T2/T1 = 750-350/750 = 0.53 (reocurring).

 

Then I move onto the final part which I am not sure about.

 

I note that the isothermal work done in expansion is an identity with the heat taken in.

 

The heat taken in Qh = mRT1In(r) Noting this problem is in specific terms I have negated m as mass of air is not given (as a punt although the units come out as desired following this approach).

 

Ergo:

 

187.5 kJ/kg = R*T1*In(r) 

 

= 0.287*750*In(r)

187.5 =215.25*In(r)

0.871=In(r)

0.871= log (base e) (V2/V1)

e^0.871 = V2/V1 

e^0.871 = 2.389

 

Then I have taken that for an isothermal process P1*V1/T1 = P2*V2/T2. T will cancel as Temerature is constant in an isothermal process leaving P1*V1 = P2*V2

 

This can then be rearanged to give P1/P2 = V2/V1 

 

Ergo: P1/P2 = 2.389 

 

As I have P1 (800 kN/m^2) I can derive P2 as 334.9 kN/m^2.

 

Or at least this is my thinking.

 

A

I was not, am not, accusing you of cheating.  And I applaud your desire to learn.  There are those (unscrupulous scalawags) who post to this forum trying to lure someone into doing their work for them; the standard response is, "Show me what you've tried."

 

There are experts in this forum that can/will help you--I'm happy to see Valerie post an example, this is one of his areas of expertise.

awibroe
14-Alexandrite
(To:Fred_Kohlhepp)

Thanks Fred,

Really appreciate that and all the support you've given me over the years. I am genuinely just thirsty for knowledge.

I've looked at V's comment but am finding it really hard to follow without context.

Cheers,

Andy.


@awibroe wrote:
Thanks Fred,


I've looked at V's comment but am finding it really hard to follow without context.

Cheers,

Andy.

See please http://www.springer.com/gp/book/9783319266732

 

awibroe
14-Alexandrite
(To:ValeryOchkov)

Gotta love a sales pitch.

I think I get the concept of using a solve block in this scenario. I could set limitations and then ask to find P2.

A
awibroe
14-Alexandrite
(To:awibroe)

Valery,

Were your diagrams for PV and TS made in MathCaD?

Andy

Try please this Mathcad Web sheet with Carno Cycle calculation with 2D and 3D diagrams

http://twt.mpei.ac.ru/MCS/Worksheets/Thermal/carno.xmcd

Carno.png

and more http://twt.mpei.ac.ru/TTHB/2/tdceng.html

And one picture in my office

Carnot.gif

I agree!

 

Looks like homework to me.  Let's see the try.

May be one example with Otto cycle help you

29-3-Otto-numerical.png29-1-Otto-plot.png

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