Energy Transfer by Heat, Work and Mass
ENERGY TRANSFER BY HEAT, WORK, AND MASS
Goal
- Identify forms of energy interactions and ways of representing it in thermodynamic processes.
Objectives
- Identify forms of energy interactions and ways of representing it in thermodynamic processes.
- Identify the types of dynamic energies interacting with a system.
- Distinguish the difference and relate between heat transfer and thermal energy.
- Write the different symbols and the conventions used to represent heat transfer.
- Differentiate between heat transfer and work.
- Write the symbols and convention used for work done.
- Obtain a mathematical relation representing mechanical work done for any system.
- Obtain the amount of work done from a P-V or P-ν graph.
- Write down the relationship between mass and volume flow rate.
- Obtain a mathematical relation representing mass flow rate in terms of mass velocities and the system’s inlet or exit area.
- Write the specific energy carried by a flowing mass.
- Use all mathematical relations and graphing skills to solve problems involving interaction energies.
Types of Energy
- Dynamic Interactions:
- Heat, Q
- Work, W
- Energy of moving mass, E_{mass}
- These forms cross in and out of the system’s boundary.
- Static System Energies:
- Internal energy, U
- Kinetic energy, KE
- Potential energy, PE
- These changes occur within the system.
Introduction
- When considering a closed adiabatic system (e.g., a sealed room with a refrigerator or fan), the only energy interaction is the electrical energy entering the room.
- Electrical energy converted into thermal energy leads to a rise in room temperature.
- E.g., a fan in a sealed room raises the temperature.
ENERGY TRANSFER BY HEAT
- Definition of Heat: The form of energy that is transferred between two systems or between a system and its surroundings due to a temperature difference.
- Example Scenarios:
- A cold soda warms up on a table.
- A hot baked potato cools down on the same table.
- Thermal Equilibrium: Energy transfer occurs until thermal equilibrium is established, moving from higher to lower temperatures.
Heat Transfer
- Definition of Heat Transfer: Energy in transition due to temperature difference, not associated with mass transfer.
- Energy is recognized as heat only when crossing the system boundary.
- Key Equations:
- Heat transfer to a system: ext{+ } ext{d}Q = Q_{in}
- Heat transfer from a system: ext{- } ext{d}Q = Q_{out}
- Heat transfer per unit mass: q = rac{Q}{m} (in unit: kJ/kg)
- Rate of heat transfer: Q = rac{Q}{t} (in units: kJ/s = kW)
- Adiabatic Process: ext{d}Q = 0. No heat transfer occurs between the system and its surroundings.
Heat Transfer Examples and Calculations
- Isothermal Process: Monitored heat transfer during constant temperature conditions; involves observing systems at known pressure and temperature states.
- Schematic and Symbols:
- For total heat entering: Q_{in} = 100 ext{ kJ}, m = 5 ext{ kg}, q_{in} = rac{Q_{in}}{m}
- For total heat leaving: Q_{out} = 20 ext{ kJ}, m = 5 ext{ kg}, q_{out} = rac{Q_{out}}{m}
- Net Heat Transfer: Q_{net} = Q_{in} - Q_{out}
ENERGY TRANSFER BY WORK
- Definition of Work: The energy transfer associated with a force acting through a distance.
- Examples of work interactions include a rising piston or rotating shaft.
- Work Sign Convention:
- Heat transfer to a system and work done on a system are positive; heat transfer from a system and work done by a system are negative.
- Symbols and Conventions:
- Electrical work when N coulombs of charge move through a potential difference V yields electrical work done.
- Mechanical Work Equation:
- Work done is represented as W = F imes d, where F is force and d is distance.
Mechanical Work and Flow Work
- Moving Boundary Work: Work associated with expansion or compression of gas in a piston-cylinder device.
- Boundary Work Calculation:
- ext{W}_{b} = ext{F} imes ext{d}s; as dV changes.
- Flow Work: Required to maintain fluid flow; W_{f} = P imes V, where P is pressure and V is volume.
- Total Energy of a Flowing Fluid:
- Total energy consists of three parts for a non-flowing fluid and four parts for a flowing fluid:
- h = u + Pv for a non-flowing fluid.
- Also includes flow work for a flowing fluid.
Energy Analysis of Steady-Flow Systems
- Operational under steady conditions where the mass and energy content of a control volume remains constant.
- Mass Conservation in Flow:
- m_{in} - m_{out} = 0 under steady-state, mass must be conserved.
Exercises
- Example Exercise: An insulated electric oven is heated through its element. Determine if this is a heat or work interaction.
- For the second exercise regarding just the air in the oven, assess the nature of energy interaction again.
Conclusion
- Understanding the principles of energy transfer through heat, work, and mass is crucial for analyzing thermodynamic systems and processes efficiently.
- Familiarity with specific terms, equations, and conditions helps in solving related thermodynamic problems, which are prevalent across multiple engineering fields.