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Second Law of Thermodynamics
Second Law of Thermodynamics
Second Law of Thermodynamics
Overview
The second law of thermodynamics builds upon the first law (conservation of energy) by adding constraints on how energy transactions can occur.
A process that satisfies the first law may not take place unless it also satisfies the second law.
Key Objectives
Understand the concept of the second law of thermodynamics.
Recognize valid processes according to thermodynamic laws.
Differentiate between thermal energy reservoirs, reversible and irreversible processes, heat engines, refrigerators, and heat pumps.
Comprehend the Kelvin–Planck and Clausius statements of the second law.
Major Uses of the Second Law
Direction of Processes
The second law helps determine the direction in which natural processes occur.
Quality of Energy
Energy has both quality (related to the second law) and quantity (related to the first law).
Quality refers to the degree of energy degradation during a process.
Performance Limits
It provides theoretical limits for the performance of engineering systems like heat engines and refrigerators.
Thermal Energy Reservoirs
Definition
A thermal energy reservoir is a hypothetical body with large thermal energy capacity that can absorb or supply heat without a temperature change.
Examples
Large bodies of water (oceans, lakes)
Atmospheric air
Two-phase systems
Heat Engines
Functionality
Heat engines convert heat into work through the following process:
Receive heat from a high-temperature source.
Convert a portion of this heat to work.
Reject remaining heat to a low-temperature sink.
Operate on a cyclic process.
Working Fluid
Typically involves a fluid for heat transfer during cycles.
Key Terms
Heat Transfers
Q_{in}: Heat supplied to the working fluid from a high-temperature source.
Q_{out}: Heat rejected to a low-temperature sink.
W_{out}: Work output from the engine.
W_{in}: Work required to compress fluids.
Thermal Efficiency of a Heat Engine
Efficiency Formula
ext{Thermal Efficiency} ( ext{η}
{th}) = rac{W
{net,out}}{Q_{in}}
Also expressed as ext{η}
{th} = 1 - rac{Q
{out}}{Q_{in}}
Waste Energy
A heat engine must reject some energy to function properly; a heat rejection process is crucial for completing the cycle.
Kelvin–Planck Statement
Definition
It states that it's impossible for any cyclic device to convert heat from a single reservoir into work without rejecting some heat.
No engine can achieve 100% thermal efficiency due to inherent limitations, not just dissipative effects.
Refrigerators and Heat Pumps
Purpose
Refrigerators transfer heat from a low-temperature medium to a high-temperature medium.
Refrigeration Cycle
Typically employs the vapor-compression refrigeration cycle.
Coefficient of Performance (COP)
For refrigerators:
ext{COP}
{R} = rac{Q
{L}}{W_{net,in}}
For heat pumps:
ext{COP}
{HP} = rac{Q
{H}}{W_{in}}
Efficiency Expression
ext{COP}
{R} = rac{Q
{L}}{Q
{H}-Q
{L}}
ext{COP}
{HP} = rac{Q
{H}}{Q
{H}-Q
{L}}
Example Calculations
Focus on practical applications for determining COP and efficiency.
Irreversible Processes
Definition of Irreversible Process
A process that cannot be reversed without changes to the surroundings.
Causes of Irreversibility
Factors like friction, unrestrained expansion, mixing fluids, and finite temperature differences cause irreversibilities.
Reversible Processes
Types:
Internally reversible: No irreversibilities occur within the system.
Externally reversible: No irreversibilities occur outside the system.
Totally reversible: No irreversibilities at all.
The Carnot Cycle
Carnot Principles
The cycle is an idealized engine cycle which is totally reversible.
Efficiency of Carnot Engines
Involves considering high and low temperature reservoirs:
ext{η}
{th} = 1 - rac{T
{L}}{T_{H}}
Applications
Understanding the Carnot efficiency helps analyze the theoretical limits of actual heat engines.
Summary of Key Statements
Key Equations
Efficiency in Heat Engines
: ext{η}
{th} = 1 - rac{T
{L}}{T_{H}}
Refrigerator Efficiency
: ext{COP}
{R} = rac{Q
{L}}{W_{in}}
Heat Pump Efficiency
: ext{COP}
{HP} = rac{Q
{H}}{W_{in}}
Understanding Relationships
Thermal efficiency and coefficient of performance showcase energy conversion limits in thermodynamic systems.
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