Chapter 5- The second law of thermodynamics

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47 Terms

1
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What is the formula for a small change in entropy, dS for a reversible process?

dQrev​ = the reversible heat flow

T= the temperature.

<p>dQ<sub>rev</sub>​ = the reversible heat flow </p><p>T= the temperature.</p>
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What does the First Law of Thermodynamics determine in a process?

It determines the energetic possibility of a process by ensuring energy conservation.

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What does the First Law of Thermodynamics restrict?

  • It restricts what processes are energetically possible by conserving energy

  • It does not specify the direction of the process.

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What does the Second Law of Thermodynamics determine?

  • It determines the direction in which a process occurs

  • It favours an increase in the entropy of the Universe.

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Why can't heat spontaneously flow from a cold body to a hot body?

  • It would decrease the entropy of the cold object more than it increases the entropy of the hot object

  • This would result in a net decrease in the total entropy of the Universe, which violates the Second Law.

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What ensures the spontaneous flow of heat from hot to cold bodies?

  • The Second Law ensures that processes spontaneously increase the total entropy of the system and surroundings

  • It favours heat flow from hot to cold bodies.

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What happens to the entropy of the Universe when Tcold<Thot?

The entropy of the Universe increases when heat flows from a hot body to a cold body

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What is a heat engine?

Its a device that uses heat to generate mechanical work by carrying a working substance through a cyclic process.

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What is the function of a heat engine?

In one cycle, the heat engine:

  1. Receives heat Q1 from a high-temperature reservoir.

  2. Emits heat Q2​ to a low-temperature reservoir.

  3. Does work w on its surroundings.

<p>In one cycle, the heat engine:</p><p></p><ol><li><p>Receives heat Q<sub>1</sub> from a high-temperature reservoir.</p></li><li><p>Emits heat Q<sub>2​</sub> to a low-temperature reservoir.</p></li><li><p>Does work w on its surroundings.</p></li></ol><p></p>
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<p>What are the sign conventions for heat and work in a heat engine?</p>

What are the sign conventions for heat and work in a heat engine?

  • Q1​: Positive (heat absorbed by the system).

  • Q2​: Negative (heat released by the system).

  • w: Negative (work done by the system on the surroundings).

<ul><li><p>Q<sub>1​</sub>: Positive (heat absorbed by the system).</p><p></p></li><li><p>Q<sub>2</sub>​: Negative (heat released by the system).</p><p></p></li><li><p>w: Negative (work done by the system on the surroundings).</p></li></ul><p></p>
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What is a Carnot heat engine?

  • An idealized heat engine that operates on an ideal gas through four reversible steps

  • Its the most efficient heat engine possible.

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Describe the working mechanism of a Carnot heat engine.

  • The Carnot engine consists of a hypothetical cylinder with a frictionless piston.

  • It operates using an ideal gas as the working fluid.

  • The engine undergoes four reversible steps that return the working fluid to its initial state.

<ul><li><p>The Carnot engine consists of a hypothetical cylinder with a frictionless piston.</p><p></p></li><li><p>It operates using an ideal gas as the working fluid.</p><p></p></li><li><p>The engine undergoes four reversible steps that return the working fluid to its initial state.</p></li></ul><p></p>
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Why is the Carnot heat engine considered ideal?

Because it represents the maximum possible efficiency achievable by a heat engine operating between two temperature reservoirs.

<p>Because it represents the maximum possible efficiency achievable by a heat engine operating between two temperature reservoirs.</p>
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What are the 4 steps in the Carnot engine cycle?

1) Reversible isothermal expansion of the gas from State A to State B

2) Reversible adiabatic expansion of the gas from State B to State C.

3) Reversible isothermal compression of the gas from State C to State D

4) Reversible adiabatic compression of the gas from State D to State A

<p>1) Reversible isothermal expansion of the gas from State A to State B</p><p></p><p>2) Reversible adiabatic expansion of the gas from State B to State C.</p><p></p><p>3) Reversible isothermal compression of the gas from State C to State D</p><p></p><p>4) Reversible adiabatic compression of the gas from State D to State A</p>
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<p>What happens during the first step of the Carnot cycle?</p>

What happens during the first step of the Carnot cycle?

Reversible isothermal expansion:

  • The gas expands from State A to State B.

  • Work w1 is done by the gas on the surroundings.

  • Heat Q1 is absorbed from the high-temperature reservoir.

  • Temperature T1​ of the gas remains constant.

<p><strong>Reversible isothermal expansion</strong>:</p><ul><li><p>The gas expands from State A to State B.</p><p></p></li><li><p>Work w<sub>1</sub> is done by the gas on the surroundings.</p><p></p></li><li><p>Heat Q1 is absorbed from the high-temperature reservoir.</p><p></p></li><li><p>Temperature T<sub>1​ </sub>of the gas remains constant.</p></li></ul><p></p>
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<p>What happens during the second step of the Carnot cycle?</p>

What happens during the second step of the Carnot cycle?

Reversible adiabatic expansion:

  • The gas expands from State B to State C.

  • The piston and cylinder are thermally isolated, so no heat is gained or lost.

  • Work w2​ is done by the gas on the surroundings.

  • The gas temperature drops to T2

<p><strong>Reversible adiabatic expansion</strong>:</p><ul><li><p>The gas expands from State B to State C.</p><p></p></li><li><p>The piston and cylinder are thermally isolated, so no heat is gained or lost.</p><p></p></li><li><p>Work w<sub>2​ </sub>is done by the gas on the surroundings.</p><p></p></li><li><p>The gas temperature drops to T<sub>2</sub></p></li></ul><p></p>
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<p>What happens during the third step of the Carnot cycle?</p>

What happens during the third step of the Carnot cycle?

Reversible isothermal compression:

  • The gas is compressed from State C to State D.

  • The surroundings do work w3​ on the gas.

  • Heat Q2 flows out of the gas to the low-temperature reservoir.

  • Temperature T2 of the gas remains constant.

<p><strong>Reversible isothermal compression</strong>:</p><ul><li><p>The gas is compressed from State C to State D.</p><p></p></li><li><p>The surroundings do work w<sub>3</sub>​ on the gas.</p><p></p></li><li><p>Heat Q<sub>2</sub> flows out of the gas to the low-temperature reservoir.</p><p></p></li><li><p>Temperature T<sub>2</sub> of the gas remains constant.</p></li></ul><p></p>
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<p>What happens during the fourth step of the Carnot cycle?</p>

What happens during the fourth step of the Carnot cycle?

Reversible adiabatic compression:

  • The gas is compressed from State D to State A.

  • The surroundings do work w4​ on the gas.

  • No heat is exchanged.

  • The gas temperature increases back to T1

<p><strong>Reversible adiabatic compression</strong>:</p><p></p><ul><li><p>The gas is compressed from State D to State A.</p><p></p></li><li><p>The surroundings do work w<sub>4​ </sub>on the gas.</p><p></p></li><li><p>No heat is exchanged.</p><p></p></li><li><p>The gas temperature increases back to T<sub>1</sub></p></li></ul><p></p>
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How is reversibility ensured in the first step of the Carnot cycle?

The temperature of the high-temperature reservoir is only infinitesimally higher than the gas temperature T1.

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How is reversibility ensured in the third step of the Carnot cycle?

The temperature of the low-temperature reservoir is only infinitesimally lower than the gas temperature T2

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How is the Carnot cycle completed?

The fourth step brings the gas back to its initial state at temperature T1 completing the cyclic process.

<p>The fourth step brings the gas back to its initial state at temperature T<sub>1</sub> completing the cyclic process.</p>
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What is the expression for the internal energy change (ΔU) during Step 1 of the Carnot cycle (Isothermal Expansion(dT=0))?

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What is the expression for the internal energy change (ΔU) during Step 2 of the Carnot cycle (Adiabatic Expansion(dQ=0))?

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24
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What is the expression for the internal energy change (ΔU) during Step 3 of the Carnot cycle (Isothermal Compression(dT=0))?

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25
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What is the expression for the internal energy change (ΔU) during Step 4 of the Carnot cycle (Adiabatic Compression(dQ=0))?

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Why is the total change in internal energy over one complete Carnot cycle zero?

The gas returns to its initial state after the cycle, so ΔUcy=0

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What is the total work (wcy​) done by the Carnot engine in a complete cycle?

Q1​ = the heat absorbed from the high-temperature reservoir

Q2​ = is the heat rejected to the low-temperature reservoir.

<p>Q<sub>1​ </sub>= the heat absorbed from the high-temperature reservoir</p><p>Q<sub>2​ </sub>= is the heat rejected to the low-temperature reservoir.</p>
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What does the first law of thermodynamics state about the Carnot cycle?

The total heat exchange is equal to the total work done in one cycle.

<p>The total heat exchange is equal to the total work done in one cycle.</p>
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Why is wcy​ negative for the Carnot engine?

  • The engine does work on the surroundings

  • This makes wcy​ negative by convention.

30
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How is the efficiency (ε) of a heat engine defined?

It is the ratio of the work done on the surroundings to the heat input at the higher temperature

<p>It is the ratio of the work done on the surroundings to the heat input at the higher temperature</p>
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32
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What is the simplified expression for the efficiency of a Carnot heat engine in terms of the heats?

Q1​ = the heat absorbed from the hot reservoir

Q2​= the heat rejected to the cold reservoir.

<p>Q1​ = the heat absorbed from the hot reservoir </p><p></p><p>Q2​= the heat rejected to the cold reservoir.</p>
33
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What is the range of values for the efficiency (ε) of a Carnot engine?

It is always less than 100%.

<p>It is always less than 100%.</p>
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What is the goal for improving the efficiency of a Carnot engine?

We aim to reduce the magnitude of the heat rejected to the cold reservoir (Q2​).

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Is it possible to reduce Q2​ (the heat rejected to the cold reservoir) to zero in a Carnot engine?

No

This is a limitation of the second law of thermodynamics.

36
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What does the second law of thermodynamics state about the efficiency of heat engines?

  • Its impossible to construct a heat engine that is 100% efficient

  • This is because some heat must always be rejected to the cold reservoir.

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What is the Kelvin Statement of the second law of thermodynamics?

"No process is possible whose sole result is the complete conversion of heat into work."

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What is the Clausius Statement of the second law of thermodynamics?

"No process is possible whose sole result is the transfer of heat from a colder to a hotter body."

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Are the Kelvin and Clausius Statements consistent with each other?

Yes. If one of them is true, then the other is also true.

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What is the heat exchange for Step 1 (Isothermal Expansion) of the Carnot cycle?

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What is the relationship for temperature and volume during Step 2 (Adiabatic Compression) of the Carnot cycle?

γ= the adiabatic index.

<p>γ=  the adiabatic index.</p>
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What is the heat exchange for Step 3 (Isothermal Compression) of the Carnot cycle?

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What is the relationship for temperature and volume during Step 4 (Adiabatic Compression) of the Carnot cycle?

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What is the key relationship between heat exchange and temperature during the Carnot cycle?

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45
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What is the thermodynamic definition of temperature?

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46
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What formula expresses the efficiency (ϵ) of a Carnot engine in terms of temperatures?

T1​= the temperature of the high-temperature reservoir

T2=​ the temperature of the low-temperature reservoir.

<p>T1​= the temperature of the high-temperature reservoir </p><p></p><p>T2=​ the temperature of the low-temperature reservoir.</p>
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How can high efficiencies be achieved in a Carnot engine?

By minimizing the ratio T2/T1:

Make T1​ as high as possible and T2 close to room temperature.