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Question: Two litres of an ideal gas at a pressure of 10 \[atm\] expands isothermally into vacuum until its to...

Two litres of an ideal gas at a pressure of 10 atmatm expands isothermally into vacuum until its total volume is 10 litres.
1.How much heat is absorbed and how much work is done in the expansion.
2.If the same expansion takes place against a constant external pressure of 1atm?
3.If the same expansion takes place to a final volume of 10 litres conducted reversibly?

Explanation

Solution

Thermodynamics is the branch of science that deals with heat, work done, temperature and transfer of energy from one form to another. The first law of thermodynamics states that energy is conserved and can neither be created nor be destroyed.

Formula used:
First law states that ΔU=QW\Delta U = Q - W. Work done is W=PΔVW = - P\Delta V and work done for reversible reaction is Wrev=2.303PVlogVfVi{W_{rev}} = - 2.303PV\log \dfrac{{{V_f}}}{{{V_i}}}

Complete step-by-step answer: We have already learnt the hint that the first law of thermodynamics highlights the law of conservation of energy. The first law states that energy can neither be created nor be destroyed but can be converted from one form to another form, it is always conserved.
Let us know about this in detail. The relationship between heat and other forms of energy is determined under the branch of science. It explains that thermal energy is converted to other forms of energy and used for various purposes. It also deals with work, temperature and energy and the transfer of energy from one place to another.
ΔU=QW\Delta U = Q - W
Where ΔU\Delta U is the change in internal energy and QQ is the added heat and WW is the work done.
Work is the process done by a system and it is not contained in a system. In thermodynamics, work done by a system is the energy transferred by the system to its surroundings. It is calculated by the formula W=PΔVW = - P\Delta V where PP is the pressure and ΔV\Delta V is the change in volume. The work done for a reversible reaction is given by Wrev=2.303PVlogVfVi{W_{rev}} = - 2.303PV\log \dfrac{{{V_f}}}{{{V_i}}}
For the above question,
1. Work is done by the system during expansion
We know that W=PΔVW = - P\Delta V
It is given that gas is expanding in vacuum which means P=0P = 0
Thus, W=0W = 0
So no work is done.
We know that the first law of thermodynamics states that ΔU=QW\Delta U = Q - W
It is given that the system is isothermal (ΔT=0\Delta T = 0), that menas ΔU=0\Delta U = 0
So, Q=W=0Q = W = 0. Hence no heat is absorbed.
2. We know that,
W=PΔVW = - P\Delta V, where

P=1atm ΔV=10.2=8L  P = 1atm \\\ \Delta V = 10.2 = 8L \\\

So, W=1×8=8atmLW = - 1 \times 8 = - 8atmL
As, Q=WQ = - W
We get, Q=(8)=8atmLQ = - ( - 8) = 8atmL
3. According to the question, work done is reversible. The expression used will be;
Wrev=2.303PVlogVfVi{W_{rev}} = - 2.303PV\log \dfrac{{{V_f}}}{{{V_i}}}
Given:

P=1atm Vf=10L Vi=8L  P = 1atm \\\ {V_f} = 10L \\\ {V_i} = 8L \\\

So,

Wrev=2.303×1×10log102 Wrev=2.303×1×10log5 Wrev=16.1J  {W_{rev}} = - 2.303 \times 1 \times 10\log \dfrac{{10}}{2} \\\ {W_{rev}} = - 2.303 \times 1 \times 10\log 5 \\\ {W_{rev}} = - 16.1J \\\

As,

Qrev=Wrev Qrev=16.1atmL  {Q_{rev}} = - {W_{rev}} \\\ {Q_{rev}} = 16.1atmL \\\

Note: An ideal gas refers to a gas whose molecules do not attract or repel each other and the only interaction between the molecules is the elastic collision due to impact of each other or the elastic collision of the molecules with the walls of the container in which the gas is stored.