Title: Sections 2.12.7
1Sections 2.1-2.7
2What happens here?
3Forms of Energy
- Total Energy Sum of all the Energies in a
system - Thermal
- Mechanical
- Kinetic
- Potential
- Electric
- Magnetic
- Chemical
- Nuclear
4Energy per unit mass
5Forms of Energy
- Internal Energy, U Sum of all of the
microscopic forms of energy.
6Mass Flow rate
7Energy of Closed/Open Systems
- Only two forms of energy associated with closed
system - Heat Transfer driven by temperature difference
- Work everything else
- Open system adds
- Energy transfer by mass flow
8Flow work
- For open systems, obviously work must be done to
move the fluid into and out of the control
volume. - It is a form of boundary work.
L
Flow
piston of fluid having m, P, V. A is
crossectional area of pipe.
9Forms of Energy
- Mechanical Energy forms of energy that can be
converted to mechanical work completely by an
ideal mechanical device - Kinetic
- Potential
- Flow Work (pressure acting on fluid over a
distance)
10Example Wind Energy
- A site evaluated for a wind farm is observed to
have steady winds at a speed of 8.5 m/s.
Determine the wind energy (a) per unit mass, (b)
for a mass of 10 kg, and (c) for a flow rate of
11.43 kg/sec for air.
11Energy Transfer by Heat
- Heat Form of energy that is transferred between
systems by the virtue of temperature difference
12Adiabatic No heat transfer
- Can happen two ways
- System is well insulated or
- System and the surrounding are at the same
temperature
13Heat Equations
kJ or BTU
kJ/sec kW
For variable heat flow
For constant heat flow
14Heat Transfer Mechanisms
- Conduction transfer of heat between more
energetic particles of a substance and less
energetic ones as a result of the interaction of
the particles (ex two solid surfaces) - Convection transfer between a solid surface and
an adjacent fluid in motion - Radiation transfer of heat due to the emission
of electro magnetic waves.
15Energy Transfer by Work
- Work Energy that crosses a system boundary that
is not heat is work - Also work is the energy transfer associated with
a force acting over a distance.
16Heat and work are directional
17Sign Conventions
- W gt 0 Work done by the system (Wout)
- W lt 0 Work done on the system (Win)
- Q gt 0 Heat Transfer to the system (Qin)
- Q lt 0 Heat transfer from the system (Qout)
18Heat and work are directional
- Qin gt 0
- Qout lt 0
- Win lt 0
- Wout gt 0
19Example Candle
- A candle is burning in a well-insulated room.
Taking the room (the air and the candle) as the
system, determine (a) if there is any heat
transfer during this burning process and (b) if
there is any change in the internal energy in the
system.
20Example Baked Potato
- A potato initially at room temperature (25oC) is
being baked in an oven that is maintained at
200oC. Is there any heat transfer during this
process?
21Example Oven
- A well-insulated electric oven is being heated
through its heating element. If the entire oven,
including the heating element, is taken to be the
system, determine whether this is a heat or work
interaction. - Answer the question again if the system is taken
as only the air in the oven without the heating
element.
22Heat and Work are Path Dependent
- Path functions have inexact differentials
designated by the symbol d. - A differential amount of heat or work is
represented by dW or dQ, instead of dW or dQ. - Properties are point functions. They have exact
differentials.
23The magnitude of path functions depend on the
path followed.
24Notes on Heat and Work
- Both are boundary phenomena.
- Systems possess energy, not heat or work.
- Both are associated with a process and not a
state. Heat has no meaning at a state. - Both are path functions.
25Types of Work
- Electrical Work
- Mechanical Work
- Shaft Work
- Work on Elastic Solid Bars
- Spring Work
- Work to stretch a liquid film
- Work to raise or accelerate a body
- Note Please review these in your text!
26First Law of ThermodynamicsConservation of Energy
- Energy can neither be created nor destroyed
during a process, it can only change forms. - The increase in the internal energy of a
thermodynamic system is equal to the amount of
heat energy added to the system minus the work
done by the system on the surroundings.
27Mechanisms of Energy Transfer
- Heat Transfer
- Work Transfer
- Mass Flow
28Conservation of EnergyFirst Law of Thermodynamics
Viewed in this way, E on the left hand side is a
property of the system. However, the right side
has Q and W which depend on the path, in general.
29Conservation of EnergyFirst Law of Thermodynamics
- Consider a closed, adiabatic system.
0
0
adiabatic
closed
30Conservation of EnergyFirst Law of Thermodynamics
- So for an adiabatic closed system the work is
equal to a path independent quantity, which means
adiabatic work is independent of path. - This is another form of the first law
- For all adiabatic processes between two
specified states of a closed system, the work is
the same, regardless of the nature of the closed
system and the details of the process.
31Energy Balance
- Look at energy entering and leaving system
- 2) Look at change in energy between two states
32Example Fan
- A fan that consumes 20W of electric power when
operating is claimed to discharge air from a
ventilated room at a rate of 1.0 kg/sec at a
discharge velocity of 8 m/s. Is this reasonable??
33NOTE THE CONVERSION TO GET FROM m2/s2 to kJ/kg
REMEMBER IT! YOU WILL NEED IT.
34Example Another Fan
- A room is initially at the outdoor temperature of
25oC. Now a large fan that consumes 200W of
electricity when running is turned on. The heat
transfer rate between the room and the outdoor
air is given as - Where U 6 W/m2/oC is the overall heat transfer
coefficient, A 30 m2 is the exposed surface
area of the room, and T1 and T0 are the indoor
and outdoor air temperatures, respectively.
Determine the indoor air temperature when steady
operating conditions are established.
35Energy Efficiency
36Hot Water Heater Purchase??
- High-Efficiency Electric 95
- High-Efficiency Gas 65
- Energy Costs
- 0.095 / kWH (electricity)
- 1.4 / Therm (gas)
- Assume heating water takes 300 kWH each month