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CHAPTER 2aCHAPTER 2a
ENERGY, ENERGY TRANSFER & GENERAL ENERGY ANALYSIS
ENERGY, ENERGY TRANSFER & GENERAL ENERGY ANALYSIS
2
CONTENTSCONTENTS
Forms of Energy
Energy Transfer by Heat
Energy Transfer by Work
Mechanical Forms of Work
The First Law of Thermodynamics
Energy Conversion Efficiencies
3
LESSON OBJECTIVESLESSON OBJECTIVES
At the end of this lesson, you should be able to:
State the various forms of energy
Describe the nature of internal energy
Describe the energy transfer by heat and work
Explain mechanical work
5
FORMS OF ENERGYFORMS OF ENERGY
Energy exists in numerous forms (thermal, mechanical, chemical, kinetic, potential, electric, magnetic & nuclear)
The sum of the energies is the total energy, E (kJ) Or for a unit mass,
Grouping of Energy forms
macroscopic
microscopic
energy of a system as a whole with respect to some outside reference frames, e.g. KE, PE
• related to molecular structure of a system and the degree of molecular activity
• independent of outside reference frames• The sum is the Internal Energy, U
m
Ee (kJ/kg)
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FORMS OF ENERGY (cont’d)FORMS OF ENERGY (cont’d)
Kinetic energy (KE)
- result of motion relative to some
reference frame (unit J)
where
= velocity of the system relative to
some fixed reference frame (m/s)
m = mass of an object (kg)
Potential energy (PE)- due to elevation in a gravitational
field (unit J)
where
g = gravitational acceleration, 9.81 m/s2
h = elevation of center of gravity of a system relative to some arbitrarily plane (m)
Macroscopic forms of energy
212212
2
2
1
2
1
mKEKEKE
mKE
mgzPE
1212 zzmgPEPEPE
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Sensible Energy
- Kinetic energy of moleculesLatent Energy- Associated with
phase of a system
Microscopic forms of energy
Chemical energy: The internal energy associated with the atomic bonds in amolecule.Nuclear energy: The tremendous amount of energy associated with the strong bonds within the nucleus of the atom itself.
The internal energy of a system is the sum of all forms of the microscopic energies.
Internal = Sensible + Latent + Chemical + Nuclear
Thermal = Sensible + Latent
FORMS OF ENERGY (cont’d)FORMS OF ENERGY (cont’d)
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Total Energy of a system
mgzmUPEKEUE 2
2
1
gzupekeue 2
2
1
Total Energy of a system per unit mass
Most of the closed system remains stationary, so for that system;
FORMS OF ENERGY (cont’d)FORMS OF ENERGY (cont’d)
Energy in Closed SystemEnergy in Closed System
Most of the closed systemremains stationary, so for that system;
0 PEKE
PEKEUE
Energy Interaction
Forms of energy not stored in the system
It is also called dynamic forms of energy
Recognized as it crosses boundary, represent energy lost or gain
The only two forms of energy interactions associated with a closed system are heat transfer and work.
The difference between heat transfer and work: An energy interaction is heat transfer if its driving force is a temperature difference. Otherwise it is work.
Energy can cross the boundaries of a closed system in the form of heat and work.
FORMS OF ENERGY (cont’d)FORMS OF ENERGY (cont’d)
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ENERGY TRANSFER BY HEATENERGY TRANSFER BY HEAT
Heat Transfer Means of energy transfer caused by temperaturedifference between the system and the surroundings
Direction of heat transfer: Higher T to Lower T
Energy is recognized as heat transfer only as it crosses the system boundary
Temperature difference is the driving force for heat transfer. The larger the temperature difference, the higher is the rate of heat transfer.
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ENERGY TRANSFER BY HEAT (cont’d)
ENERGY TRANSFER BY HEAT (cont’d)
Adiabatic process is a process during which there is no heat transfer, Q=0
How a process can be adiabatic?
Well insulated system
No temperature difference
Adiabatic is not necessarily means isothermal process. Temperature of the system can still be changed by other means
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Amount of heat transferred is denoted by Q (kJ)
For a unit mass:
m
Qq (kJ/kg)
Q positive indicates heat inputQ negative indicates heat lost
Sign Convention for Heat:
Specifying the directions of heat using in and out
ENERGY TRANSFER BY HEAT (cont’d)
ENERGY TRANSFER BY HEAT (cont’d)
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MECHANISMS OF HEAT TRANSFER
Conduction Convection Radiation
The transfer of energy due to the emission of electromagnetic waves (or photons).
The transfer of energy from the more energetic particles of a substance to the adjacent less energetic ones as a result of interaction between particles.
The transfer of energy between a solid surface and the adjacent fluid that is in motion, and it involves the combined effects of conduction and fluid motion.
ENERGY TRANSFER BY HEAT (cont’d)
ENERGY TRANSFER BY HEAT (cont’d)
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ENERGY TRANSFER BY WORKENERGY TRANSFER BY WORK
Work is an energy interaction between a system and its surroundings that is not caused by temperature difference
WORK Energy transfer associated with a force acting through a distance, e.g. rotating shaft, rising piston
The work done by, or on, a system is defined as (unit kJ):
2
1
.s
sdsFW or
m
Ww Work done per unit mass
The work done per unit time is Power (unit kJ/s or kW):
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Sign convention for work:
The work done by, or on, a system is defined as (unit kJ):
W positive indicates work done by system (work output)W negative indicates work done on the system (work input)
Specifying the directions of work using in and out
ENERGY TRANSFER BY WORK (cont’d)ENERGY TRANSFER BY WORK (cont’d)
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Heat vs. Work
Both are recognized at the boundaries of a system as they cross the boundaries. That is, both heat and work are boundary phenomena.
Systems possess energy, but not heat or work.
Both are associated with a process, not a state.
Unlike properties, heat or work has no meaning at a state.
Both are path functions (i.e., their magnitudes depend on the path followed during a process as well as the end states).
Properties are point functions; but heat and work are path functions (their magnitudes depend on the path followed).
ENERGY TRANSFER BY WORK (cont’d)ENERGY TRANSFER BY WORK (cont’d)
19
Electrical power in terms of resistance R, current I, and potential difference V.
Electrical work
Electrical power
When potential difference and current change with time
When potential difference and current remain constant
ENERGY TRANSFER BY WORK (cont’d)ENERGY TRANSFER BY WORK (cont’d)
20
MECHANICAL FORMS OF WORKMECHANICAL FORMS OF WORK
There are two requirements for a work interaction between a system and its surroundings to exist:
there must be a force acting on the boundary.
the boundary must move.
Work = Force Distance When force is not constant
If there is no movement, no work is done.
In thermo, most of the work is mechanical work, which associated with moving boundary work
Other common forms of workShaft workSpring work
21
A force F acting through a moment arm r generates a torque T
Shaft work is proportional to the torque applied and the number of revolutions of the shaft.
This force acts through a distance s
The power transmitted through the shaft is the shaft work done per unit time
Shaft work:
SHAFT WORKSHAFT WORK
22
When the length of the spring changes by a differential amount dx under the influence of a force F, the work done is:
For linear elastic springs, the displacement x is proportional to the force applied
k: spring constant (kN/m)
Substituting and integrating yield
x1 and x2: the initial and the final displacements
The displacement of a linear spring doubles when the force is doubled.
SPRING WORKSPRING WORK
23
Different forms of work transfer could occur in a system simultaneously during a process.
The total or net work done by the system = algebraic sum of all work
NET WORK DONE BY A SYSTEMNET WORK DONE BY A SYSTEM
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