Thermofluids: Change in energy

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Discussion Overview

The discussion revolves around a thermofluids problem involving a gas in a closed rigid tank with an electric resistor providing energy input and heat transfer to the surroundings. Participants explore the implications of energy transfer rates, the relationship between work and heat, and the mathematical modeling of energy changes over time.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants express confusion regarding the equation for heat transfer, Q[SIZE="1"](dot) = -50t, questioning how it can be in watts when multiplied by time in minutes.
  • One participant mentions using the equation dE/dt = Q[SIZE="1"](dot) - W[SIZE="1"](dot) and describes their approach of analyzing two closed systems to understand energy transfer.
  • Another participant clarifies that the resistor creates heat through "I squared R" heating, explaining the relationship between current, resistance, and heat generation.
  • There is a discussion about whether the resistor should be classified as a work transfer source or a heat transfer source, with some participants referencing differing interpretations from textbooks.
  • One participant successfully completes part 'a' of the problem but seeks further clarification on the role of the resistor in energy transfer.
  • Another participant emphasizes the importance of the 1000 watts input in the context of energy changes within the system.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the classification of the resistor's energy input as work or heat transfer, indicating a lack of agreement on this conceptual point. Additionally, there are varying interpretations of the equations and their implications for the problem.

Contextual Notes

Participants express uncertainty regarding the mathematical relationships and definitions involved in the problem, particularly concerning the units of heat transfer and the nature of energy input from the resistor.

Who May Find This Useful

This discussion may be useful for students and practitioners in thermodynamics, engineering, and physics who are grappling with concepts of energy transfer, heat generation, and the application of the first law of thermodynamics in closed systems.

johnsonc007
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1. The problem at hand: A gas is contained in a closed rigid tank. An electric resistor in the tank transfers energy to the gas at a constant rate of 1000W. Heat transfer between the gas and the surroundings occurs at a rate of Q(dot) = -50t, where Q (dot) is in watts, and t is in time, minutes.
(a) Plot the time rate of change of energy of the gas for 0<t<20 min in watts. (actually t is greater than or equal to 0, and t is less than or equal to 20)
(b) Determine the net change in energy of the gas after 20 minutes, in kJ



2. I am not following on how to complete this task. I am confused by the Q(dot) equation. How can it equal watts when multiplied by minutes, as a watt is a J/s? Would get Q(dot)=Jmin/s...


3. I have tried to solve this numerous times, all with the wrong solution. I tried starting part b first as I need that data to do part a. I know that dE/dt = Q(dot) - W(dot). I drew two closed systems, one with the gas isolated with the resistor work entering and Q=0, and then another with the resister in the system and Q leaving the system, so that W=0. Am I on the right path? If so, what can I do with that? I found W=1200kJ but Q being some huge number and not working towards the correct solution.
Also took derivatives, but that got me nowhere fast too :(
 
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johnsonc007 said:
1. The problem at hand: A gas is contained in a closed rigid tank. An electric resistor in the tank transfers energy to the gas at a constant rate of 1000W. Heat transfer between the gas and the surroundings occurs at a rate of Q(dot) = -50t, where Q (dot) is in watts, and t is in time, minutes.
(a) Plot the time rate of change of energy of the gas for 0<t<20 min in watts. (actually t is greater than or equal to 0, and t is less than or equal to 20)
(b) Determine the net change in energy of the gas after 20 minutes, in kJ



2. I am not following on how to complete this task. I am confused by the Q(dot) equation. How can it equal watts when multiplied by minutes, as a watt is a J/s? Would get Q(dot)=Jmin/s...


3. I have tried to solve this numerous times, all with the wrong solution. I tried starting part b first as I need that data to do part a. I know that dE/dt = Q(dot) - W(dot). I drew two closed systems, one with the gas isolated with the resistor work entering and Q=0, and then another with the resister in the system and Q leaving the system, so that W=0. Am I on the right path? If so, what can I do with that? I found W=1200kJ but Q being some huge number and not working towards the correct solution.
Also took derivatives, but that got me nowhere fast too :(
As time goes on, the tank surface temperature increases and so does the heat that escapes. Thus, the power input as a function of time is:

Q(t) = 1000 watt - 50 (watt / min ) t

For example, when t = 5 min, the energy that is absorbed inside the tank is:

Q(5 min) = 1000 watt - 50 (watt / min) 5 min = 750 watt

The total energy absorbed is: Energy = power X time or E = P t or dE = P dt

and E = Integral (Q (t) ) dt
 
Ok. Totally makes sense for part 'a', actually figured it out last night with a study partner.

Now for part 'b': I was considering that the resistor input was work transfer, not heat transfer. Why is the resistor considered a heat transfer source?

Your assistance helped me finish the problem, thank you! However I would like a better understanding of the relationship of the resistor to the energy of the gas and the system. Can you clarify? (The textbook associated with this class showed a resistor as a work source, not heat. It must have been just for that example.)
 
johnsonc007 said:
Ok. Totally makes sense for part 'a', actually figured it out last night with a study partner.

Now for part 'b': I was considering that the resistor input was work transfer, not heat transfer. Why is the resistor considered a heat transfer source?

Your assistance helped me finish the problem, thank you! However I would like a better understanding of the relationship of the resistor to the energy of the gas and the system. Can you clarify? (The textbook associated with this class showed a resistor as a work source, not heat. It must have been just for that example.)
The resister creates heat by what is called "I squared R" heating. In other words, when you pass a current I (in amps) through a resistance R (in ohms) you release heat Q = I^2 R in watts. This is why most of the power consumption of an incandescent light bulb goes into heat.

In this problem, the 1000 watt source could come from passing 10 amps of current through a 10 ohm resister (or any other combination of I^2 R that gives 1000 watt). As far as the energy is concerned, 1000 w is important.

Now from the 1st law of thermo, we simply have (ignoring changes in kinetic and potential energy): Qheat = m (hf - hi) = m cp (Tf - Ti). We could then find the temperature of the gas, Tf, as a function of time by solving the first law equation for Tf and with Qheat = Integral Qheat(t) dt.

Usually a work source will have shaft rotation (e.g turbine, pump, fan, windmill, and so on).
 

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