Finding heat exchanged work done to compress gas

In summary: It makes it a little easier to remember when you are studying for an exam.Thank you for your reply @Chestermiller! That is a good method that I have not seen before!
  • #1
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Homework Statement
For this part(b) of this problem:

When a gas expands along AB (see below), it does 20 J of work and absorbs 30 J of heat. When the gas expands along AC, it does 40 J of work and absorbs 70 J of heat. (a) How much heat does the gas exchange along BC? (b) When the gas makes the transition from C to A along CDA, 60 J of work are done on it from C to D. How much heat does it exchange along CDA?

The solution is ##90J##. However, I am getting ##30J##. My working is

##\Delta E_{int_{CDA}} = -\Delta E_{int_{CA}} = -30 ##
##-30 = Q - (-60) ##
## 30 J = Q ##

Can some please let me know what I am doing wrong?

Many thanks!
Relevant Equations
First Law of Thermodynamics ##\Delta E_{int} = Q - W##
1680316124814.png
 
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  • #2
If
##-30 = Q - (-60)##,
what do you get when you move ##(-60)## to the left side and change the sign that is in front of it outside the parentheses? Alternatively, get rid of the parentheses first, then move the term over.
 
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  • #3
kuruman said:
If
##-30 = Q - (-60)##,
what do you get when you move ##(-60)## to the left side and change the sign that is in front of it outside the parentheses? Alternatively, get rid of the parentheses first, then move the term over.
Thank you for your reply @kuruman !

##-30 = Q + 60##
##-90 = Q##

But the solution is ##90 = Q##. Thank you, I guess I messed up in the algebra there, but is the reason why in their answer ##Q > 0## because there are only concerned when the heat exchanged so we don't need to say that the heat is loss from the system?

Many thanks!
 
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  • #4
The easiest way to do this is to take point A as the datum of zero internal energy: ##E_A=0##. Then $$E_B=30-20=10\ J$$
$$E_C=70-40=30\ J$$So $$E_A-E_C=-30=Q+60$$
 
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  • #5
ChiralSuperfields said:
Thank you for your reply @kuruman !

##-30 = Q + 60##
##-90 = Q##

But the solution is ##90 = Q##. Thank you, I guess I messed up in the algebra there, but is the reason why in their answer ##Q > 0## because there are only concerned when the heat exchanged so we don't need to say that the heat is loss from the system?

Many thanks!
Yes. It's the magnitude of the heat that flows between the environment and gas regardless of where this heat starts and ends up. There are four ways to say the same thing:
  1. The heat that leaves the gas and enters the environment is 90 J
  2. The heat that enters the environment from the gas is 90 J.
  3. The heat that leaves the environment and enters the gas is - 90 J.
  4. The heat that enters the gas from the environment is -90 J.
These can be summarized with loss of direction information as "The heat that is exchanged between gas and environment is 90 J." By convention, the ##Q## in the first law of thermodynamics is chosen to represent the heat that enters the gas from the environment, option 4.
 
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  • #6
Chestermiller said:
The easiest way to do this is to take point A as the datum of zero internal energy: ##E_A=0##. Then $$E_B=30-20=10\ J$$
$$E_C=70-40=30\ J$$So $$E_A-E_C=-30=Q+60$$
Thank you for your reply @Chestermiller ! That is a good method that I have not seen before!
 
  • #7
kuruman said:
Yes. It's the magnitude of the heat that flows between the environment and gas regardless of where this heat starts and ends up. There are four ways to say the same thing:
  1. The heat that leaves the gas and enters the environment is 90 J
  2. The heat that enters the environment from the gas is 90 J.
  3. The heat that leaves the environment and enters the gas is - 90 J.
  4. The heat that enters the gas from the environment is -90 J.
These can be summarized with loss of direction information as "The heat that is exchanged between gas and environment is 90 J." By convention, the ##Q## in the first law of thermodynamics is chosen to represent the heat that enters the gas from the environment, option 4.
Thank you for your reply @kuruman!

That is quite interesting all those combinations of saying the same thing!
 

FAQ: Finding heat exchanged work done to compress gas

What is the formula for calculating the work done to compress a gas?

The work done to compress a gas is given by the formula \( W = -\int_{V_i}^{V_f} P \, dV \), where \( W \) is the work done, \( P \) is the pressure, and \( V_i \) and \( V_f \) are the initial and final volumes, respectively. For an ideal gas undergoing an isothermal process, this can be simplified to \( W = nRT \ln\left(\frac{V_f}{V_i}\right) \), where \( n \) is the number of moles, \( R \) is the gas constant, and \( T \) is the temperature.

How do you determine the heat exchanged during the compression of a gas?

The heat exchanged during the compression of a gas can be determined using the first law of thermodynamics, which states \( \Delta U = Q - W \). Here, \( \Delta U \) is the change in internal energy, \( Q \) is the heat added to the system, and \( W \) is the work done by the system. For an ideal gas, if the process is isothermal, \( \Delta U = 0 \), thus \( Q = W \). For adiabatic processes, \( Q = 0 \), and the change in internal energy is equal to the work done on the gas.

What is the difference between isothermal and adiabatic compression?

In isothermal compression, the temperature of the gas remains constant throughout the process. This means that any work done on the gas results in heat being transferred out of the system to maintain the temperature. In adiabatic compression, no heat is exchanged with the surroundings, so all the work done on the gas increases its internal energy, resulting in a rise in temperature.

How does the specific heat capacity of a gas affect the heat exchanged during compression?

The specific heat capacity of a gas determines how much heat is required to change the temperature of a given amount of gas. During compression, if the process is not isothermal or adiabatic, the specific heat capacities at constant volume \( C_v \) and at constant pressure \( C_p \) are used to calculate the change in internal energy and the heat exchanged. For example, in a polytropic process, the heat exchanged can be calculated using \( Q = nC_v(T_f - T_i) + W \), where \( T_i \) and \( T_f \) are the initial and final temperatures.

What role does the gas constant (R) play in the calculations of work done and heat exchanged?

The gas constant \( R \) is a fundamental constant that appears

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