Thermofluids: Change in energy

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SUMMARY

The discussion centers on a thermofluids problem involving a gas in a closed rigid tank with an electric resistor transferring energy at a constant rate of 1000W. Heat transfer is described by the equation Q(dot) = -50t, where Q(dot) represents heat loss in watts over time in minutes. Participants clarified the relationship between work and heat transfer, concluding that the resistor acts as a heat source due to "I squared R" heating. The net change in energy after 20 minutes can be calculated using the first law of thermodynamics, integrating the power input and heat loss over time.

PREREQUISITES
  • Understanding of the first law of thermodynamics
  • Familiarity with heat transfer concepts, specifically "I squared R" heating
  • Basic knowledge of calculus for integration and differentiation
  • Ability to interpret power equations in thermodynamic systems
NEXT STEPS
  • Study the first law of thermodynamics and its applications in closed systems
  • Learn about heat transfer mechanisms, particularly conduction and convection
  • Explore the concept of "I squared R" heating and its implications in electrical systems
  • Practice solving thermodynamic problems involving energy transfer and heat loss
USEFUL FOR

Students and professionals in mechanical engineering, thermodynamics, and energy systems, particularly those working with heat transfer and energy conservation 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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