Termodinamika – problemos ir sprendimai

Termodinamika – problemos ir sprendimai

Pirmasis termodinamikos dėsnis

1. Remiantis toliau pateiktu PV grafiku, koks yra santykis darbas kokį darbą dujos atliko I procese, kokį darbą dujos atliko II procese?

Žinomas:Termodinamika – problemos ir sprendimai 1

1 procesas:

Slėgis (P) = 20 N/m²2

Pradinis tūris (V1) = 10 litrų = 10 dm3 = 10 x 10-3 m3

Galutinis tūris (V2) = 40 litrų = 40 dm3 = 40 x 10-3 m3

2 procesas:

Process (P) = 15 N/m2

Pradinis tūris (V1) = 20 litrų = 20 dm3 = 20 x 10-3 m3

Galutinis tūris (V2) = 60 litrų = 60 dm3 = 60 x 10-3 m3

Ieškoma: The ratio of the work done by gas

sprendimas:

The work done by gas in the process I :

W = P ΔV = P (V2– V1) = (20)(40-10)(10-3 m3) = (20)(30)(10-3 m3) = (600)(10-3 m3) = 0.6 m3

The work done by gas in the process II :

W = P ΔV = P (V2– V1) = (15)(60-20)(10-3 m3) = (15)(40)(10-3 m3) = (600)(10-3 m3) = 0.6 m3

The ratio of the work done by gas in the process I and the process II :

0.6 m3 : 0.6 m3

1: 1

2.

Based on the graph below, what is the work done by helium gas in the process AB?

Termodinamika – problemos ir sprendimai 2Žinomas:

Pressure (P) = 2 x 105 N / m2 = 2 x 105 Paskalis

Pradinis tūris (V1) = 5 cm3 = 5 x 10-6 m3

Galutinis tūris (V2) = 15 cm3 = 15 x 10-6 m3

Ieškoma: Work done by gas in process AB

sprendimas:

W = ∆P ∆V

W = P (V2 - V1)

W = (2 x 105)(15 x 10-6 - 5 x 10-6)

W = (2 x 105)(10 x 10-6) = (2 x 105)(1 x 10-5)

W = 2 džaulių

3.

Based on the graph below, what is the work done in process a-b?

Termodinamika – problemos ir sprendimai 3Žinomas:

Initial pressure (P1) = 4 Pa = 4 N/m2

Final pressure (P2) = 6 Pa = 6 N/m2

Pradinis tūris (V1) = 2 m3

Galutinis tūris (V2) = 4 m3

Ieškoma: work done I process a-b

sprendimas:

Work done by gas = area under curve a-b

W = area of triangle + area of rectangle

W = ½ (6-4)(4-2) + 4(4-2)

W = ½ (2)(2) + 4(2)

W = 2 + 8

W = 10 džaulių

4. Based on graph below, what is the work done in process A-B-C-A.

sprendimas:

Termodinamika – problemos ir sprendimai 4Work (W) = Area of the triangle A-B-C

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W = ½ (20-10)(6 x 105 - 2 x 105)

W = ½ (10)(4 x 105)

W = (5)(4 x 105)

P = 20 x 105

P = 2 x 106 Džaulio

Šilumos variklis

5. An engine absorbs 2000 Joule of heat at a high temperature and exhausted 1200 Joule of heat at a low temperature. What is the efficiency of the engine?

Žinomas:

Šilumos tiekimas (QH) = 10 000 džaulių

Šilumos išeiga (QL) = 10 000 džaulių

Work done by engine (W) = 2000 – 1200 = 800 Joule

Ieškoma: efficiency (e)

sprendimas:

e = W / QH

e = 800/2000

e = 0.4 x 100%

e = 40 %

Karno variklis

6. An engine absorbs heat at 960 Kelvin and the engine discharges heat at 576 Kelvin. What is the efficiency of the engine.

Žinomas:

Aukšta temperatūra (TH) = 960 K

Žema temperatūra (TL) = 576 K

Ieškoma: efficiency (e)

sprendimas:

Termodinamika – problemos ir sprendimai 5

Efficiency of Carnot engine = 0.4 x 100% = 40%

7. Based on the graph below, work done by the engine is 6000 Joule. What is the heat discharged by engine each circle?

Žinomas:Termodinamika – problemos ir sprendimai 6

Darbas (W) = 6000 džaulis

Aukšta temperatūra (TH) = 800 Kelvin

Žema temperatūra (TL) = 300 Kelvin

Ieškoma: heat discharged by the engine

Sprendimas :

Carnot (ideal) efficiency :

Termodinamika – problemos ir sprendimai 7

Heat absorbed by Carnot engine :

W = eQ1

6000 = (0.625) Q1

Q1 = 6000/0.625

Q1 = 9600

Heat discharged by Carnot engine :

Q2 = Q1 - W

Q2 = 9600 - 6000

Q2 = 2 376 000 džaulių

8. The efficiency of a Carnot engine is 40%. If heat absorbed at 727°C then what is the low temperature.

Žinomas:

Efficiency (e) = 40% = 40/100 = 0.4

Aukšta temperatūra (TH) = 727oC + 273 = 1000 K

Ieškoma: Žema temperatūra

sprendimas:

Termodinamika – problemos ir sprendimai 8

TL = 600 Kelvin – 273 = 327oC

9. Based on graph below, if the engine absorbs 800 J of heat, what is the work done by the engine.

Žinomas:Termodinamika – problemos ir sprendimai 9

Aukšta temperatūra (TH) = 600 Kelvin

Žema temperatūra (TL) = 250 Kelvin

Šilumos tiekimas (Q1) = 10 000 džaulių

Ieškoma: Darbas (W)

sprendimas:

The efficiency of Carnot engine :

Termodinamika – problemos ir sprendimai 10

Work was done by the engine :

W = eQ1

W = (7/12)(800 Joule)

W = 466.7 džaulių

10. The high temperature of a Carnot engine is 600 K. If the engine absorbs 600 J of heat and the low temperature is 400 K, what is the work done by the engine.

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Žinomas:

Žema temperatūra (TL) = 400 K

Aukšta temperatūra (TH) = 600 K

Šilumos tiekimas (Q1) = 10 000 džaulių

Ieškoma: Darbą atliko Carnot variklis (W)

sprendimas:

Carnot variklio efektyvumas:

Termodinamika – problemos ir sprendimai 11

Work was done by Carnot engine :

W = eQ1

W = (1/3)(10 000) = 200 džaulių

  1. What is the primary focus of thermodynamics? atsakymas: Thermodynamics focuses on the study of energy, its transformations, and its relationship with matter, especially in systems at equilibrium.
  2. How is the zeroth law of thermodynamics related to temperature? atsakymas: The zeroth law states that if two systems are each in thermal equilibrium with a third system, then they are in thermal equilibrium with each other. This implies the existence of a property called temperature, which is the same for all systems in thermal equilibrium.
  3. What does the first law of thermodynamics describe? atsakymas: The first law, also known as the law of energy conservation, states that energy cannot be created or destroyed, only converted from one form to another. In a closed system, the change in internal energy is equal to the heat added to the system minus the work done by the system on its surroundings.
  4. Why is the second law of thermodynamics crucial for understanding the direction of natural processes? atsakymas: The second law states that the entropy (or disorder) of an isolated system always increases or remains constant. This dictates that energy spontaneously disperses if not hindered from doing so, providing a direction to natural processes and essentially explaining why certain processes occur spontaneously while others do not.
  5. What is entropy, and how does it relate to disorder in a system? atsakymas: Entropy is a measure of the amount of energy in a system that is unavailable to do work. It is also often described as a measure of the system’s disorder or randomness. In general, higher entropy corresponds to greater disorder or randomness.
  6. How does the third law of thermodynamics describe the entropy of a perfect crystal at absolute zero? atsakymas: The third law states that the entropy of a perfect crystal is exactly zero at absolute zero temperature (0 Kelvin). This means that at this temperature, the system is perfectly ordered.
  7. Why can’t heat flow from a colder body to a hotter body on its own? atsakymas: This behavior is a consequence of the second law of thermodynamics. If heat were to flow from a colder body to a hotter one spontaneously, it would lead to a decrease in the overall entropy of the system, which is not favored by natural processes.
  8. What is the difference between an isolated, closed, and open system in thermodynamics? atsakymas: An isolated system does not exchange energy or matter with its surroundings. A closed system can exchange energy but not matter with its surroundings. An open system can exchange both energy and matter with its surroundings.
  9. How is the concept of “work” in thermodynamics different from the everyday use of the term? atsakymas: In thermodynamics, “work” refers to the process of energy transfer where forces applied to an object move it in a direction parallel to the force. For example, when a gas expands against a piston, it does work on the piston. This is a more specific definition compared to the everyday use of “work,” which might simply mean any task or activity.
  10. What is a Carnot cycle, and why is it significant in thermodynamics? atsakymas: The Carnot cycle is an idealized thermodynamic cycle that provides an upper limit on the efficiency that any classical thermodynamic engine can achieve during the conversion of heat into work (or vice versa). It’s significant because it sets a fundamental efficiency limit based on the temperatures of the heat reservoirs between which an engine operates.