Tuesday 30 August 2016

Gate 2016 
Thermodynamics Questions
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Dear friends while going through gate paper of this year, I came across one problem which many of my students find difficult to solve, the problem was of Vapour compression cycle but when you look critically the problem it can't be solved without applying thermodynamics to it. So you can see how deceptive sometimes the problem can be.

Lets look the problem first:

Now let us see how to solve this problem:



so you see how important thermodynamics is. If you know thermodynamics then RAC, Power plant and Heat transfer will become cake walk for you all.

Few more problems from same set:




Now solutions of above problems:





Now few problems from set 2(you can see the problems in IISC Gate site)



Few problems from set 1:


Now solutions of above problems:




Prepare well 
All the Best

Monday 29 August 2016


I. E. Irodov

 First law of Thermodynamics, Heat Capacity 

Solutions


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Friends do not get surprise by looking the heading of today's post. The story behind today's post started in the year 2002 when I was preparing for IIT-JEE examinations. In those days it was a trend that if you can solve I. E. Irodov then you can crack JEE, but because of lack of knowledge and very short duration of preparation in which I have to finish my text books also I failed in solving Irodov. But today I am in a situation to solve it and I strongly recommend this book for all those student out there who are preparing for GATE and ESE. For mechanical engineering students I strongly recommend following sections of this book:

1.1  Kinematics
1.2  Fundamental equations of Dynamics
1.3  Laws of Conservation of Energy, Momentum, and Angular Momentum
1.5 Dynamics of a Solid Body
1.6  Elastic Deformations of a Solid Body
1.7  Hydrodynamics
2.2  The First Law of Thermodynamics. Heat Capacity
2.4  The Second Law of Thermodynamics. Entropy
2.5  Liquids. Capillary Effects
2.6  Phase Transformations
2.7  Transport Phenomena 


Dear friends in this post I will be solving section 2.2 and in later post I will be solving Section 2.4 as they are the topics of this blog. the solutions of section 1.7 I have already uploaded in Slideshare and the link is there in one of the pages in my blog.

Point to be noted here is that I have solved the problems in mass bases not mole basis as well I have solved the problems as if they are derivation and if you want to arrive at the final answer which is given in book so please substitute the values and you will get the answer. There are few problems whose ans. I have not given I will be providing them in few days, so stay connected.

I have converted the problems in mass basis and in the form of derivative problem so they are different in form but same in concept with the problems in books

Let us start the solving the problems:

26.  Demonstrate that the interval energy U of the air in a room is independent of temperature provided the outside pressure p is constant. Calculate U, if p is equal to the normal atmospheric pressure and the room's volume is equal to V = 40 m3.


     28.  Two thermally insulated vessels 1 and 2 are filled with air and connected by a short tube equipped with a valve. The volumes of the vessels, the pressures and temperatures of air in them are known (V1, p1, T1 a nd V2, p2, T2). Find the air temperature and pressure established after the opening of the valve.


    29.  Gaseous hydrogen contained initially under standard conditions in a sealed vessel of volume V  was cooled by ΔT .  Find how much the internal energy of the gas will change and what amount of heat will be lost by the gas.


30.  What amount of heat is to be transferred to nitrogen in the isobaric heating process for that gas to perform the work W ?

      31.  As a result of the isobaric heating by ΔT m kg of a certain ideal gas obtains an amount of heat Q . Find the work performed by the gas, the increment of its internal energy, and the value of γ = Cp/Cv.

     32. m kg of a certain ideal gas at a temperature To were cooled isochorically so that the gas pressure reduced n times. Then, as a result of the isobaric process, the gas expanded till its temperature got back to the initial value. Find the total amount of heat absorbed by the gas in this process.





  35.  m kilogram of a certain ideal gas is contained under a weightless piston of a vertical cylinder at a temperature T. The space over the piston opens into the atmosphere. What work has to be performed in order to increase isothermally the gas volume under the piston it times by slowly raising the piston? The friction of the piston against the cylinder walls is negligibly small.



 37.  m kilogram of an ideal gas being initially at a temperature To were isothermally expanded n  times its initial volume and then isochorically heated so that the pressure in the final state became equal to that in the initial state. The total amount of heat transferred to the gas during the process equals . Find the ratio γ = Cp/Cv for this gas.

 38.  Draw the approximate plots of isochoric, isobaric, isothermal, and adiabatic processes for the case of an ideal gas, using the following variables:
(a) p, T; (b) V, T.





 39. One kilogram of oxygen being initially at a temperature To  is adiabatically compressed to increase its pressure η times. Find:
(a) the gas temperature after the compression;
(b) the work that has been performed on the gas.


    40.  A certain mass of nitrogen was compressed η  times (in terms of volume), first adiabatically, and then isothermally. In both cases the initial state of the gas was the same. Find the ratio of the respective works expended in each compression.


 43.  The volume of m kilogram of an ideal gas with the adiabatic exponent γ is varied according to the law V = a / T, where a is a constant. Find the amount of heat obtained by the gas in this process if the gas temperature increased by ΔT.


 44.  Demonstrate that the process in which the work performed by an ideal gas is proportional to the corresponding increment of its internal energy is described by the equation pVn = const, where n is a constant.


  45.  Find the heat capacity of an ideal gas in a polytropic process pVn = const if the adiabatic exponent of the gas is equal to γ. At what values of the polytropic constant n will the heat capacity of the gas be negative?


  46.  In a certain polytropic process the volume of argon was increased α times. Simultaneously, the pressure decreased β times. Find the heat capacity of argon in this process, assuming the gas to be ideal.


  47.  m kilogram of argon is expanded polytropically, the polytropic constant being n . In the process, the gas temperature changes by ΔT . Find:
(a) the amount of heat obtained by the gas;
(b) the work performed by the gas

  48.  An ideal gas whose adiabatic exponent equals γ is expanded so that the amount of heat transferred to the gas is equal to the decrease of its internal energy. Find:
(a) the heat capacity of the gas in this process;
(b) the equation of the process in the variables T, V;
(c) the work performed by one mole of the gas when its volume increases η times if the initial temperature of the gas is To.


   49.  m kilogram of an ideal gas whose adiabatic exponent equals γ undergoes a process in which the gas pressure relates to the temperature as p = aTα, where  a and α are constants. Find:
(a) the work performed by the gas if its temperature gets an increment ΔT;
(b) the heat capacity of the gas in this process; at what value of α will the heat capacity be negative?



  50.  An ideal gas with the adiabatic exponent γ undergoes a process in which its internal energy relates to the volume as U=aVα, where a and α are constants. Find:
(a) the work performed by the gas and the amount of heat to be transferred to this gas to increase its internal energy by ΔU;
              (b) the heat capacity of the gas in this process.


 51.   An ideal gas has a heat capacity Cv at constant volume. Find the molar heat capacity of this gas as a function of its volume V, if the gas undergoes the following process:
(a)    T=T0 eαV  (b)P=P0 eαV,    where Po, To, and α are constants.


  52.  m kilogram of an ideal gas whose adiabatic exponent equals γ undergoes a process p = po + a /V, w here Po and a are positive constants. Find:
(a) heat capacity of the gas as a function of its volume;
(b) the internal energy increment of the gas, the work performed by it, and the amount of heat transferred to the gas, if its volume increased from V1 to V2.


  53.  m kg  of an ideal gas with heat capacity at constant pressure Cp undergoes the process T = To +α V, where T o and α are constants. Find:
(a) heat capacity of the gas as a function of its volume;
(b) the amount of heat transferred to the gas, if its volume increased from V1 to V2.



 54.  For the case of an ideal gas find the equation of the process (in the variables T, V) in which the heat capacity varies as:
(a) C = Cv + αT; (b) C = Cv + βV; (c) C = Cv + ap,
where α, β, and a are constants.


  55.  An ideal gas has an adiabatic exponent γ. In some process its heat capacity varies as C = α/T, where a is a constant. Find:
(a) the work performed by one mole of the gas during its heating from the temperature To to the temperature η times higher;
(b) the equation of the process in the variables p, V.

      56.  Find the work performed by one mole of a Van der Waals gas during its isothermal expansion from the volume V1 to V2 at a temperature T.





 57.  m kilogram of oxygen is expanded from a volume V1 to V2  at a constant temperature T . Calculate:
(a) the increment of the internal energy of the gas:
 (b) the amount of the absorbed heat.
The gas is assumed to be a Van der Waals gas.

  58.  For a Van der Waals gas find:
(a) the equation of the adiabatic curve in the variables T, V;
(b) the difference of the heat capacities Cp, — Cv as a function
of T and V.


  59.  Two thermally insulated vessels are interconnected by a tube equipped with a valve. One vessel of volume V1  contains m  of carbon dioxide. The other vessel of volume V 2 is evacuated. The valve having been opened, the gas adiabatically expanded. Assuming the gas to obey the Van der Waals equation, find its temperature change accompanying the expansion.


60. What amount of heat has to be transferred to m Kg of carbon dioxide to keep its temperature constant while it expands into vacuum from the volume V1  to V 2 ? The gas is assumed to be a Van der Waals gas.


  61.  What amount of heat has to be transferred to m kg of carbon dioxide to keep its temperature constant while it expands into vacuum from the volume V1 to V2? The gas is assumed to be a Van der Waals gas.



One more thing I want to say ( which I say always to every student) that please do not follow the solutions blindly. Firstly try yourself and if find difficulty in solving, then only look the solutions.
After few days I will be publishing solutions of next section (i.e. 2.4 --The Second Law of Thermodynamics. Entropy)

your comments are valuable to me, so please do write them. If any problem in any solution then also let me know.
Thankyou
All the Best.


Saturday 27 August 2016

CHAPTER 1
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Dear friends hope that you are practicing well.
Now I am providing you with the solutions of chapter 1(Introduction)


Before I start providing you the solutions I would like to give a brief introduction of chapter.

In this chapter you have studied about macro and microscopic thermodynamics,  system and its types,  processes i.e. extensive and intensive,  Thermodynamic equilibrium and also about quasi-equilibrium process commonly known as quasi-static process.
At last you have studied about Concept of Continuum.


Dear friends for a quick review of what I said above you can click the videos below where I am giving a  quick review of this chapter:







So let us start solving problems:







This is all I have to say on this chapter. These problems are of 4th edition. 
One more thing I want to say ( which I have also mentioned in previous posts) that please do not follow the solutions blindly. firstly try yourself and if find difficulty in solving, then only look the solutions.
After few days I will be publishing solutions of chapter seven (i.e. ENTROPY ) so stay connected.

your comments are valuable to me, so please do write them. If any problem in any solution then also let me know.
Thankyou
All the Best.

Thursday 25 August 2016

CHAPTER 6
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Dear friends hope that you are practicing well.
Now I am providing you with the solutions of chapter 6(Second Law of Thermodynamics)


Before I start providing you the solutions I would like to give a brief introduction of chapter.

In this chapter you have studied about qualitative difference between low grade and High grade energy transfers along with cyclic heat engines and Thermal  energy reservoirs. you have studied 2 statements of second law i.e. Kelvin-Planck and Clausius statements. you have studied about reversibility and causes because of which a process deviates from it i.e. internal dissipation and external irreversibility. you have studied about Carnot's engine and cycle along with reversed Carnot cycle.
 You have studied about Carnot's Theorem and its corollary and based on the outcome of that you have developed absolute temperature scale.


Dear friends for a quick review of what I said above you can click the videos below where I am giving a  quick review of Second law of thermodynamics.










So let us start solving problems:






















This is all I have to say on this chapter. These problems are of 4th edition. 
One more thing I want to say ( which I have also mentioned in previous post) that please do not follow the solutions blindly. firstly try yourself and if find difficulty in solving, then only look the solutions.
After few days I will be publishing next chapter solutions so stay connected.

your comments are valuable to me, so please do write them. If any problem in any solution then also let me know.
Thankyou
All the Best.