Π£ Π½Π°Ρ Π²Ρ ΠΌΠΎΠΆΠ΅ΡΠ΅ ΠΏΠΎΡΠΌΠΎΡΡΠ΅ΡΡ Π±Π΅ΡΠΏΠ»Π°ΡΠ½ΠΎ 11/12.3 Entropy and the Second Law of Thermodynamics | General Physics ΠΈΠ»ΠΈ ΡΠΊΠ°ΡΠ°ΡΡ Π² ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡΠ½ΠΎΠΌ Π΄ΠΎΡΡΡΠΏΠ½ΠΎΠΌ ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅, Π²ΠΈΠ΄Π΅ΠΎ ΠΊΠΎΡΠΎΡΠΎΠ΅ Π±ΡΠ»ΠΎ Π·Π°Π³ΡΡΠΆΠ΅Π½ΠΎ Π½Π° ΡΡΡΠ±. ΠΠ»Ρ Π·Π°Π³ΡΡΠ·ΠΊΠΈ Π²ΡΠ±Π΅ΡΠΈΡΠ΅ Π²Π°ΡΠΈΠ°Π½Ρ ΠΈΠ· ΡΠΎΡΠΌΡ Π½ΠΈΠΆΠ΅:
ΠΡΠ»ΠΈ ΠΊΠ½ΠΎΠΏΠΊΠΈ ΡΠΊΠ°ΡΠΈΠ²Π°Π½ΠΈΡ Π½Π΅
Π·Π°Π³ΡΡΠ·ΠΈΠ»ΠΈΡΡ
ΠΠΠΠΠΠ’Π ΠΠΠΠ‘Π¬ ΠΈΠ»ΠΈ ΠΎΠ±Π½ΠΎΠ²ΠΈΡΠ΅ ΡΡΡΠ°Π½ΠΈΡΡ
ΠΡΠ»ΠΈ Π²ΠΎΠ·Π½ΠΈΠΊΠ°ΡΡ ΠΏΡΠΎΠ±Π»Π΅ΠΌΡ ΡΠΎ ΡΠΊΠ°ΡΠΈΠ²Π°Π½ΠΈΠ΅ΠΌ Π²ΠΈΠ΄Π΅ΠΎ, ΠΏΠΎΠΆΠ°Π»ΡΠΉΡΡΠ° Π½Π°ΠΏΠΈΡΠΈΡΠ΅ Π² ΠΏΠΎΠ΄Π΄Π΅ΡΠΆΠΊΡ ΠΏΠΎ Π°Π΄ΡΠ΅ΡΡ Π²Π½ΠΈΠ·Ρ
ΡΡΡΠ°Π½ΠΈΡΡ.
Π‘ΠΏΠ°ΡΠΈΠ±ΠΎ Π·Π° ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ ΡΠ΅ΡΠ²ΠΈΡΠ° ClipSaver.ru
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...