Thermodynamics First law ideal gas question

In summary, the conversation discusses the calculation of the initial temperature of an ideal gas that is expanded from an initial volume of V1 to a final volume of V2=3V1. The process is reversible and T/V is constant. The work obtained by the expansion is given as 9.4 KJ, and the value of R is 8.314 KJ Kmol-1. Two methods are presented for finding the initial temperature, with different results. The correct method involves using PΔV as the work done and solving for T1, resulting in a temperature of 721 K.
  • #1
deeko1987
7
0

Homework Statement



We have
0.0008 Kmol of an ideal gas are expanded from V1 to V2 v2=3V1
process is reversible and T/V=Constant

if the work obtained by this expansion is 9.4 KJ find the initial temperature

R=8.314 KJ Kmol-1

Homework Equations



PV=nRT

possibly T/V = T/V

The Attempt at a Solution



The method I thought to use is as follows.

PV=nRT we know work = 9.4KJ

9.4/nR = T2

T2/V2 = T1/V1

multiply T2/V2 by V1

and we get T2/3 (because the ratio is 1/3)

got 471.092 kelvin for T1

a class mate used this method

PV= 9.4KJ

Pressure is constant as t/v=constant

P(3V1-V1) = 9.4KJ

2PV1= 9.4 KJ (divide by 2)
PV1 = 4.8KJ

PV1=nRT2 = 4.8

solving for t

4.8/nR = 721

T1 = 721 kelvin

Could somebody please explain which method is correct to use and if it is the second method the how this works.In my view the work down at PV1 should not be equal to half the initial work done because the question states the work done expanding from V1 to V2. Also using the second method wouldn't that still be by definition T2 because although we have algebraically modified the
equation we still have T2 in the formula.

Many thanks
 
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  • #2
deeko1987 said:
The method I thought to use is as follows.

PV=nRT we know work = 9.4KJ
The work done equals PΔV, not PV. (When pressure is constant, of course.)
 
  • #3
deeko1987 said:
Also using the second method wouldn't that still be by definition T2 because although we have algebraically modified the
equation we still have T2 in the formula.
There should not be a T2 in the formula. The second method uses PV1 = nRT1.
 
  • #4
Actually, your class mate is right. You said that PV=nRT = 9,4 KJ, and that's not right. Remember that the general definition of work in thermodynamics is the integral of PdV. This is a isobaric process, so the expression turns to: P(Vf-Vi), or PΔV. It's the variation of volume!
Also, you used 4,8 instead of 4,7 for 2PV1= 9.4 KJ (divide by 2). I found 706 K for the initial temperature.
 
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What is the first law of thermodynamics?

The first law of thermodynamics states that energy cannot be created or destroyed, only transferred or converted from one form to another.

How does the first law of thermodynamics apply to ideal gases?

The first law of thermodynamics applies to ideal gases by stating that the internal energy of an ideal gas is directly proportional to its temperature. This means that when an ideal gas undergoes a change in temperature, the internal energy will also change.

What is an ideal gas?

An ideal gas is a theoretical gas that follows the ideal gas law, which describes the relationship between pressure, volume, and temperature. It is characterized by having particles that have no volume and do not interact with each other.

What is the ideal gas law?

The ideal gas law is a mathematical equation that describes the relationship between pressure, volume, and temperature of an ideal gas. It is written as PV = nRT, where P is pressure, V is volume, n is the number of moles, R is the gas constant, and T is temperature.

How can the first law of thermodynamics be applied to real-life situations?

The first law of thermodynamics can be applied to real-life situations, such as in the production and consumption of energy. It is also used in the design and operation of various heat engines, refrigerators, and air conditioners. Additionally, it is crucial in understanding the energy transformations that occur in chemical reactions and the behavior of different systems, such as the Earth's atmosphere and oceans.

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