2. Syst Flashcards

1
Q

A ?(1)? is a definable part of the world that is interesting to us.

It is seperated from its ?(2)? by a system boundary.

A

(1) system

(2) environment

(3) boundary

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2
Q

Thermodynamic processes can be understood as a mutual influence of system and environment or of two systems among themselves. The influence takes place by ??

A

transfer of energy

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3
Q

Name 3 types of energy transfer!

A

Mechanical

Thermal

Through material flow

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4
Q

Types of energy transfer: Mechanical

Energy in form of ?(1)? crosses the system boundary

A

work(W)

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5
Q

Types of energy transfer: Thermal

Energy in the form of ?? is transferred across the system boundaries.

A

heat (Q)

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6
Q

Types of energy transfer: through material flow

Different types of energy (e.g. ??) cross the system boundary with the material flow.

A

kinetic energy

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7
Q

General Energy balancing Formula?

A

Change in the total energy of system

(=)

Total Energy entering the system

(-)

Total Energy leaving the system

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8
Q

Elements of Thermodynamics: ?? (3)

A

System and system boundaries

State/status and variables describing the status

Process and process variables

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9
Q

State variables

Name 3 thermal and 3 caloric state variables!

A

thermal: Temp. (T), Pressure (p), Volume (V)

caloric: Internal energy (U), Enthalpy (H), Entropy (S)
-> specific jeweils mit /m

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10
Q

State variables

?(1)? -> depend on the prevailing temperature

?(2)? -> describe the energy content of a system

A

(1) thermal

(2) caloric

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11
Q

Name 4 Process variables!

A

Work: W
Power: P = dW / dt

Heat: Q
Heat flow: Qdot = dQ / dt

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12
Q

The (electrical) work done on an adiabatic system is equal to?

A

the increase in the energy of the system

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13
Q

The energy change of a system during a process is equal to?

A

the net work and heat transfer between the system and its surroundings

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14
Q

Ex1: A rigid tank contains a hot fluid that is cooled while being stirred by a paddle wheel. Initially, the internal energy of the fluid loses 500kJ of heat, and the paddle wheel does 100kJ of work on the fluid.

Determine the final internal energy of the fluid (U2). Neglect the energy stored in the paddle wheel!

A

Wsh,in - Qout = deltaU = U2 - U1

100kJ - 500kJ = U2 - 800kJ

–> U2 = 400kJ

(
For a closed system delta U = delta Q + delta W
-> if we add work or heat to the system, the internal energy will increase
-> this will result in increased state variables like temp., pressure or volume
-> A transfer of heat will result in an increase of internal energy and is proportional to the increase in temperature by a factor c

-> Attention: This does not apply to phase transition and c is not constant for the same substance across all temperature levels!
-> c is the thermal capacity of the system and it depends on the substance as well as the conditions under which the heat transfer takes place (constant p or V)
)

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15
Q

What does the Law of Conservation of Energy say?

A

The sum of all forms of energy always remains the same.

-> but: Energy = Exergy + Anergy

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16
Q

Energie = Exergy + Anergy

Welche Energie ist useful?

A

Exergy -> Anergy is not useful

17
Q

??: The part of the energy that can be converted into any other form of energy under given thermodynamic conditions of the environment.

A

Exergy (Availability)

18
Q

The exergy share ?? in all conversion processes.

19
Q

??: The part of the energy that cannot be converted into other forms of energy, e.g. thermal energy at the temperature level of the environment

20
Q

What does the 1st law of thermodynamics say?

A

Energy consumption in the thermodynamic sense does not exist, as the sum of exergy and anergy is constant.

21
Q

What does the 2nd law of thermodynamics say?

A

Energy can be degraded from exergy to anergy and it is never possible to convert anergy into exergy.

(This principle could be interpreted as energy consumption)

22
Q

?(1)? = fully usuable, unlimitedly convertible part of energy (e.g. work); entropy-free

?(2)? = non-usuable part of the energy in the considered environment; afflicted with entropy

A

(1) Exergy

(2) Anergy

(A cup of hot coffee does not get hotter in a cooler room)

23
Q

Ex. 2: A piston–cylinder device contains a liquid-vapor mixture of water at 300 K. During a constant pressure process, 750 kJ of heat is transferred to the water. As a result, part of the liquid in the cylinder vaporizes.

Determine the entropy change of the water during this process.

A

delta S system = delta Q / Tsystem

delta S system = 750 kJ / 300K = 2,5 kJ/K

Formel gilt bei konstanter Temp. und reversiblen Prozess

-> liegt hier vor, denn:

1) Der Prozess wird bei konstanter Temp. durchgeführt. delta Q wird ausschließlich dazu verwendet, die Phasenumwandlung bei konstanter Temp. und Druck zu ermöglichen.

2) Bei Phasenwechselprozessen (wie Verdampfen) unter konstantem Druck und konstanter Temp handelt es sich um quasi-statische (nahezu reversible) Prozesse.

24
Q

T-v Diagram and P-v Diagram
-> see slide 15

25
On a T-s diagram, the area under the process curve represents the ?(1)? for internally reversible processes. The isentropic process appears as a ?(2)? on a T-s diagram.
(1) heat transfer (2) vertical line -> see slide 16
26
T-s diagrams of reversible and irreversible processes -> see difference slide 17+18
...
27
A heat engine receives heat from a source at 1200K at a rate of 500 kJ/s and rejects the waste heat to a medium at 300K. The power output of the heat engine is 180kW. 1) Determine the reversible power and the irreversibility rate for this process. 2) What is the Carnot efficiency of this engine?
1) Reversible power: Wdot rev = eta th * Qdot in = (1- Tsink/Tsource) * Qdotin = (1 - 300K/1200K) * 500kW = 375kW irreversibility rate Idot: Idot = Wdot rev - Wdot real = 375 kW - 180 kW = 195 kW 2) Carnot efficiency eta c: eta c = eta th = 1 - Tsink/Tsource = 1 - 300K/1200K = 0.75 (rev. power entspricht max. theoretisch erreichbarer Leistung, wenn Prozess reversibel abläuft)
28
Rankine Cycle (Ideal Vapor Power Plant) Draw the scheme of powerplant, name all four steps and draw the T-s diagram of the ideal cycle!
see slide 22-23
29
Draw a T-s diagram of a Rankine cycle considering the irreversibilities of the components.
see slide 25
30
Ideal Rankine Cycle with a Reheater 1) Draw the scheme of the cycle! 2) Draw the T-s Diagram
see slide 27
31
How is efficiency defined?
As the ratio between the useful energy delivered and the energy input required for this. (The efficiency is a snapshot which refers to a certain (optimum) operating point)
32
Formeln: Efficiency = ?? Energy efficiency = ?? Exergetic efficiency = ??
Efficiency = I Benefits I / Effort -> with 0 <= eta <= 1 Energy efficiency = Pout / (Pin +Qin) -> etatotalen = eta1,en + eta2,en + ... + etan,en Exergetic efficiency = Ex(Pout) / (Ex(Pin) +Ex(Qin)) -> etatotal,ex = eta1,ex + eta2,ex + ... + etan,ex
33
The degree of utilization is the average efficiency determined over a longer period of time. The efficiency is therefore always ?? to the degree of utilization
higher or equal
34
80l of water at a temperature of 45°C are mixed with 10 liters of tap water at 15°C. What is the temperature of the mixture?
Heat dissipated = heat absorbed Qin = -Qout with Qout < 0 Qin = I Qout I m1c1 (T1-Tmix) = m2c2 (Tmix - T2) <=> (m1c1)/(m2c2) = (Tmix - T2) / (T1 - Tmix) <=> Tmix = (m1c1T1 + m2c2T2) / (m1c1 + m2c2) = (m1T1 + m2T2) / (m1+m2) = ((80*45+10*15) / (80*10)) °C = 41,7°C (Amount of heat always goes from body with higher temp. to body with lower temp. Amount of heat needed to heat a body from T1 to T2: Q = m * c * (T2 - T1) )
35
Rechne Task 6-12 !!! (siehe mit Lösung summ. Ex2) -> maybe noch KT
...
36
In an electrode hot water boiler, hot water is produced for a district heating network. Explain the energy conversion processes and state changes within the boiler using the 1st and 2nd thermodynamic law.
According to the 1st law, energy is always converted and not generated or destroyed: E2 - E1 = Q + W + edeltam -> Here: No work and closed system: E2 - E1 = 0 Electrical energy is converted into thermal energy by the resistance in the electrode and transferred to the water. The water heats up. The 2nd law describes the "value" of energy. Exergy is the part of energy that is usable for us (100% for electrical energy) and anergy describes the part of energy that is not usable (here, a part of the thermal energy of water) The exergy share depends on temperature levels. Entropy is generated and irreversibilities result. The thermal energy of water cannot simply be converted back into electrical energy
37
Name for each energy forms an example for ideal conversion and the exergy share of the converted energy! 1) Epot 2) Ekin 3) U (Internal energy): a) Charge energy (electricity) b) Chemical binding energy c) Thermal energy
1) Leverage , 100% 2) Impact, 100% 3a) Movement of load carriers, 100% 3b) Fuel cell, < 100% 3c) Thermal engine, << 100%