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11/12.3 Entropy and the Second Law of Thermodynamics | General Physics ΡΠΊΠ°Ρ‡Π°Ρ‚ΡŒ Π² Ρ…ΠΎΡ€ΠΎΡˆΠ΅ΠΌ качСствС

11/12.3 Entropy and the Second Law of Thermodynamics | General Physics 2 Π³ΠΎΠ΄Π° Π½Π°Π·Π°Π΄

ΡΠΊΠ°Ρ‡Π°Ρ‚ΡŒ Π²ΠΈΠ΄Π΅ΠΎ

ΡΠΊΠ°Ρ‡Π°Ρ‚ΡŒ mp3

ΡΠΊΠ°Ρ‡Π°Ρ‚ΡŒ mp4

ΠΏΠΎΠ΄Π΅Π»ΠΈΡ‚ΡŒΡΡ

Ρ‚Π΅Π»Π΅Ρ„ΠΎΠ½ с ΠΊΠ°ΠΌΠ΅Ρ€ΠΎΠΉ

Ρ‚Π΅Π»Π΅Ρ„ΠΎΠ½ с Π²ΠΈΠ΄Π΅ΠΎ

бСсплатно

Π·Π°Π³Ρ€ΡƒΠ·ΠΈΡ‚ΡŒ,

НС удаСтся Π·Π°Π³Ρ€ΡƒΠ·ΠΈΡ‚ΡŒ Youtube-ΠΏΠ»Π΅Π΅Ρ€. ΠŸΡ€ΠΎΠ²Π΅Ρ€ΡŒΡ‚Π΅ Π±Π»ΠΎΠΊΠΈΡ€ΠΎΠ²ΠΊΡƒ Youtube Π² вашСй сСти.
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11/12.3 Entropy and the Second Law of Thermodynamics | General Physics
  • ΠŸΠΎΠ΄Π΅Π»ΠΈΡ‚ΡŒΡΡ Π’Πš
  • ΠŸΠΎΠ΄Π΅Π»ΠΈΡ‚ΡŒΡΡ Π² ОК
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Π‘ΠΊΠ°Ρ‡Π°Ρ‚ΡŒ Π²ΠΈΠ΄Π΅ΠΎ с ΡŽΡ‚ΡƒΠ± ΠΏΠΎ ссылкС ΠΈΠ»ΠΈ ΡΠΌΠΎΡ‚Ρ€Π΅Ρ‚ΡŒ Π±Π΅Π· Π±Π»ΠΎΠΊΠΈΡ€ΠΎΠ²ΠΎΠΊ Π½Π° сайтС: 11/12.3 Entropy and the Second Law of Thermodynamics | General Physics Π² качСствС 4k

Π£ нас Π²Ρ‹ ΠΌΠΎΠΆΠ΅Ρ‚Π΅ ΠΏΠΎΡΠΌΠΎΡ‚Ρ€Π΅Ρ‚ΡŒ бСсплатно 11/12.3 Entropy and the Second Law of Thermodynamics | General Physics ΠΈΠ»ΠΈ ΡΠΊΠ°Ρ‡Π°Ρ‚ΡŒ Π² максимальном доступном качСствС, Π²ΠΈΠ΄Π΅ΠΎ ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠ΅ Π±Ρ‹Π»ΠΎ Π·Π°Π³Ρ€ΡƒΠΆΠ΅Π½ΠΎ Π½Π° ΡŽΡ‚ΡƒΠ±. Для Π·Π°Π³Ρ€ΡƒΠ·ΠΊΠΈ Π²Ρ‹Π±Π΅Ρ€ΠΈΡ‚Π΅ Π²Π°Ρ€ΠΈΠ°Π½Ρ‚ ΠΈΠ· Ρ„ΠΎΡ€ΠΌΡ‹ Π½ΠΈΠΆΠ΅:

  • Π˜Π½Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΡ ΠΏΠΎ Π·Π°Π³Ρ€ΡƒΠ·ΠΊΠ΅:

Π‘ΠΊΠ°Ρ‡Π°Ρ‚ΡŒ mp3 с ΡŽΡ‚ΡƒΠ±Π° ΠΎΡ‚Π΄Π΅Π»ΡŒΠ½Ρ‹ΠΌ Ρ„Π°ΠΉΠ»ΠΎΠΌ. БСсплатный Ρ€ΠΈΠ½Π³Ρ‚ΠΎΠ½ 11/12.3 Entropy and the Second Law of Thermodynamics | General Physics Π² Ρ„ΠΎΡ€ΠΌΠ°Ρ‚Π΅ MP3:


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11/12.3 Entropy and the Second Law of Thermodynamics | General Physics

Chad provides a lesson on Entropy and the Second Law of Thermodynamics. The lesson begins with a conceptual description of entropy as a measure of disorder. The Second Law of Thermodynamics is then presented showing that the entropy of the universe increases for a spontaneous process. A more formal and mathematical definition for entropy change follows along with the presentation and derivation of equations for calculating entropy for an isothermal expansion or compression as well as the demonstration that the entropy change for an adiabatic process is zero. Chad also shows how to calculate the entropy change associated with heating or cooling and solves an example calculation. Chad next presents the mathematical relationship between entropy and the number of microstates. S=kBlnW Chad shows that a system for which only 1 microstate exists will have zero entropy, and then as the number of microstates increases, so too does the entropy. Systems that have more disorder tend to also have more microstates explaining why they also have more entropy. The lesson is concluded with a discussion of heat engines and thermal efficiency. An expression for the work performed by a heat engine is presented along with an expression for calculating the thermal efficiency of a heat engine. A Carnot engine is then described as an engine with the highest possible thermal efficiency. The four steps of the Carnot Cycle are then described: 1. Isothermal Expansion 2. Adiabatic Expansion 3. Isothermal Compression 4. Adiabatic Compression It is shown how the thermal efficiency of a Carnot engine is dependent only upon the temperature of the hot reservoir (heat sink) and cold reservoir (cold sink), and that the thermal efficiency can never actually reach 100%. 00:00 Lesson Introduction 00:51 Entropy and Disorder 01:23 Second Law of Thermodynamics 05:01 Entropy Change Definition and Calculations 07:13 How to Calculate Delta S for Heating and Cooling 15:30 Entropy and Microstates 20:40 Heat Engines and Thermal Efficiency 24:38 The Carnot Cycle and Thermal Efficiency Check out Chad's General Physics Master Course: https://www.chadsprep.com/physics-you...

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