29 Engineering
29.1 Electrical
Circuits
29.1.1 Phase Locked Loop
A phase locked loop consists of a phase detector, a low-pass filter, and a
voltage-controlled oscillator (VCO). The locked output comes out of the VCO
and is fed back into the phase detector, which compares the phase with the input
signal. The larger the phase difference, the smaller the DC voltage output of
the phase detector, but there are also the extraneous original frequencies,
harmonics, and sum frequencies. The subsequent low-pass filter strips these off
forwarding the more slowly changing DC voltage. If the phase increases the
lower voltage will increase the VCO frequency until it catches up with the input
signal. If the phase decreases the higher voltage will reduce the VCO frequency
until it slows to the input signal.
Figure
29-1: Phase Locked Loop
29.1.2 Resonance
The advantage of resonance in a circuit is that it permits the circuit to
act as straight though wire at resonance. For example this permits the
selection of the ideal AC coupling capacitor.
Figure
29-2: Solving for a Resonance Capacitor or
Inductor
29.2 Electromagnetic
Fields
29.2.1 Vector Calculus
Perpendicular vectors have dot products that are zero due to the cosine(90)
being zero.
Parallel vectors have cross products that are zero due to the
sin(0) being zero. This means the magnitude of the normal is zero for parallel
vectors.
29.2.2 Maxwell’s Equations
Maxwell’s equations derive from Ampere’s law and Gauss’s
law for statics.
The integral forms derive from the Differential forms
using Stokes’ Law
[2498]
and the Divergence Law.
Equation
29-1: Stokes' Theorem
The line integral of the vector A along a closed path C is equal
to the integral of the dot product of the curl of the vector A with the normal
to the surface S that has the contour C as its boundary.
Equation
29-2: Divergence Theorem
The closed surface integral of the normal component of vector A over a
surface S is equal to the volume integral of the divergence of A over the volume
V enclosed by S.
Equation
29-3: Ampere's Law
Ampere’s law for statics is
∇ x
H =
J.
Maxwell added the electric displacement current density
Jd = ∂
D / ∂t.
The
third law of Maxwell’s equations is Gauss’s
law.
[2499]
Equation
29-4: Gauss’s Law
Electric flux flowing out of a closed surface = charge
enclosed
∫s D • dS =
∫v q dV
where the vector
dS = n*dS is a vector in the outward normal of the
surface with magnitude
dS.
[2500]
where the vector D is the Displacement Vector = Electric Flux
Density = D = ε *
E
∫ D cos
θ dS = ∫s D
• n dS = ∫s D • dS
29.2.3 Electrical Properties of Matter
Materials are:
- Dielectrics (insulators) – Polarization (electric displacement current
density) is predominant phenomenon. The formation of electric dipoles between
opposite charges of atoms or in atoms is the source of polarization.
- Magnetics – Magnetization (magnetic displacement current density) is
predominant phenomenon.
- Conductors – Conduction (conduction current density) is the
predominant phenomenon. The prominent characteristic is the motion of electric
charges and the creation of current
flow.[2501]
Polarization is in C/m2 – Coulombs per
square meter, which is a bound surface charge density
qsp.
An increase in temperature for a conductor increases
the thermal energy in its lattice structure causing lattice vibration and more
collisions for moving electrons, thus a decrease in
conductivity.
Semiconductors bridge the gap between Dielectrics and
Conductors. In intrinsic (pure) semiconductors the carriers include:
- Free electrons
- Bound electrons – positive holes
Mobility is (drift
velocity)/(unit E field). In semiconductors, drift velocity decreases with
increased temperature due to collisions. However, charge density increases with
temperature. Hence, with increase in temperature, mobility decreases, while
conductivity increases.
Table
29-1: Temperature Increase effects on
Materials
|
Drift Velocity [m/s] ve – drift velocity
of electrons ve = -
μe E where E
is V/m
|
Mobility
[m2/(V-s)] μe
– mobility of
electrons μh
– mobility of holes
|
Conductivity
|
|
Metallic Conductor
|
Electrons drift in the negative direction of an applied electric
field
|
In conductors, positive and negative charges are separated by macroscopic
distances. This is a fundamental difference between true charges in conductors
and bound charges in
dielectrics. [2502]
|
Decreases
|
|
Semiconductor
|
Decreases
|
Decreases
|
Increases
|
|
Superconductor
|
T↑ ve↑ T↓
ve↓ since E→0 T→TC (~0K)
E→0
|
Constant
|
For T→TC(~0°K)
σ→∞
TC – Critical Temperature
|
The three constitutive properties characterize the electrical property
of the material.
The permittivity –
ε indicates the storage capacity
of a material and is in (Farads/Meter). It indicates how well a material
permits an Electric field to pass through. The scale is in an inverse sense
such that a vacuum has the smallest permittivity (8.854 * 10-12) and
lets the largest E-field pass. While a higher permittivity, dielectric such as
water at 81 would serve as an excellent capacitive material in storing an
E-field for release.
The permeability –
μ indicates the inductive quality
of the material and is in (Henries/Meter). The larger the permeability the
material may store a larger magnetic field. In Free Space the permeability is
4π * 10-7
Henries/Meter.
The conductivity –
σ is the inverse ohms per meter
and indicates the charge movement quantity capability of the medium
1/(Ω Meters).
Table
29-2: Constitutive Parameters of a Material for Electrical
Characterization
|
Permittivity –
ε
|
Permeability –
μ
|
Conductivity –
σ
|
|
Units
|
Farads/Meter
|
Henries/Meter
|
Siemens/Meter or MHO/Meter or
1/(Ω Meters)
|
|
Description
|
Capacitive storage of the material as a function of frequency.
|
Inductive storage of the material as a function of frequency.
|
Charge movement capability of the medium as a function of
frequency.
|
|
Free Space Value
|
8.854 * 10-12 F/m
|
4π * 10-7
H/m
|
0 MHO/m
|
|
Relation (* denotes convolution)
|
D = ε *
E
|
B = μ *
H
|
Jc = σ
* E
|
The permeability of most dielectric material is the same as free
space.
Frequency, permittivity and conductivity that is the loss tangent
specify whether a material is a good conductor or a good
dielectric:
σ/(ωε)
>> 1 Conductor – conduction current density prevails
Jc
σ/(ωε)
<< 1 Dielectric – displacement current density prevails
Jd
where
σ/(ωε)
= tan δ
Hence, the loss
tangent tells us the operational behavior of a material at a particular
frequency.
Table
29-3: Current Density
|
A/m2
|
Name and Description
|
Equivalence
|
|
J
|
Total Current Density
|
|
|
Jc
|
Conduction Electric Current Density – Physically, conductors
are material whose outer shell valence electrons are not held tightly and
migrate from atom to atom. [2503]
These valence electrons are called free electrons, since they move
easily.
|
|
|
Jd
|
Displacement Electric Current Density – In dielectrics, the
motion of bound charges, create a true current and constitute part of the
displacement current
density. [2504] Physically the
electric flux in a region displaces a bound electron in a filled shell from an
atom or molecule, which moves to its neighbor displacing another bound electron.
The process creates a true current.
|
J d = ∂ D/∂t =
j ωD =
j ωεEthat is the
change in the Electric Flux
Density [2505] in
C/(s-m 2)
|
|
Ji
|
Impressed (source) Electric Current Density – A current source
that can create a conduction electric current density if there is a conductor or
a displacement electric current density if there is a dielectric in its
path.
|
|
|
Jm
|
Bound magnetic current density – This current density is the
direct result of polarization derived from Jms below. The
dipoles are bound in the material except for their orientation. The current
density is in a loop with the polarization in the normal direction.
|
Jm = ∇ x M (A/m2)
|
|
Jms
|
Bound Magnetic surface current density is a net result of all dipole
moments since the internal microscopic current densities
cancel. [2506] Jms
introduces the magnetization vector or
magnetic polarization vector M (A/m) that is in the
same direction as the applied magnetic field
Ba. [2507]
M tells the magnetization dipole density in the material.
|
Jms = M x
ń|surface gives the direction around the
surface
|
|
Jp
|
[2508][2509]
|
Jp = ∂P/∂t
|
The secondary properties describe the dependencies of the constitutive
parameters.
[2510] Graphically,
convolution of two waves is taking the mirror reflection of the second wave and
moving it towards the origin of the first wave, while plotting the area under
the curve as a function of time given by the slide of the
intersection.
Table
29-4: Secondary Parameters of a Material
|
Property
|
Definition
|
|
Linear
|
Constitutive properties not a function of the applied field
strength. [2511]
|
|
Nonlinear
|
Constitute properties are a function of the applied field
strength.
|
|
Homogeneous
|
Constitutive properties not a function of position in the media.
|
|
Nonhomogeneous Inhomogeneous
|
Constitutive properties are a function of position in the media.
|
|
Isotropic
|
Constitutive properties not a function of the direction of the applied
field.
|
|
Nonisotripic Anisotropic
|
Constitutive properties are a function of the direction of the applied
field. A permittivity
tensor [2512] gives the
relationship between the electric flux density and electric field in three
dimensions with D = ē
• E
|
|
Dispersive
|
Constitutive properties are a function of frequency.
|
|
Nondispersive
|
Constitutive properties not a function of frequency.
|
The electrons surrounding the nucleus of an atom also spin around their own
axis. Each contributes a
±9 E-24 magnetic
moment.
[2513] Only the
electrons found in incompletely filled shells contribute to this magnetic moment
as the ones in filled shells cancel each other out. The nucleus of an atom also
has a spin, but the nuclear spin is much smaller than the electron moment by a
factor of E-3.
Table
29-5: Magnetic Properties of Matter
|
Material Class
|
Permeability
|
Cause
|
Description
|
|
Diamagnetic
|
0.999 ≤ μr
< 1
|
Atoms or molecules with no intrinsic magnetic dipole moment are
distorted by the applied magnetic field to acquire an induced dipole
moment antiparallel with the applied
field. [2514]In the
absence of the applied field, thermal agitation randomizes the orientation and
there is no net alignment along a preferred
direction. [2515]
|
The net small magnetization vector opposes the applied magnetic field
resulting in permeability just below unity. In a magnetic field, their
induced magnetism is in a direction opposite to that of iron.
All
materials, with or without intrinsic moments are subject to the diamagnetic
distortion, but it is a weak effect easily masked by the paramagnetic alignment
when present.
|
|
Vacuum
|
μr = 1
|
|
|
|
Paramagnetic
(Antiferromagnetic - noting or pertaining to a
substance in which, at sufficiently low temperatures, the magnetic moments of
adjacent atoms point in opposite directions.)
|
1 < μr <
1.001 When applying a magnetic field dipoles align slightly producing a
small non-zero M in its direction and a small increase in the magnetic
flux density within the material.
|
Magnetic moments of spinning electrons of an atom do not cancel each other
out in the absence of an applied electric field. However, in the macroscopic
view, multiple atoms cancel each other’s magnetic moments. Above
the Curie temperature point ferromagnetic materials revert to paramagnetic
behavior. [2516]For
ferromagnetic materials, a remarkable quantum mechanical phenomenon causes the
intrinsic moments to self-align over regions of the material called
domains.
|
Net magnetization vector aids magnetic field resulting in a relative
permeability greater than 1. Also, there is a magnetic susceptibility
χm slightly
greater than 0. A body or substance that, placed in a magnetic field,
possesses magnetization in direct proportion to the field strength; a substance
in which the magnetic moments of the atoms are not aligned.
|
|
Ferrimagnetic and the subclass Ferrite
(Often from metal oxides or
ceramics – high permeability, i.e. strong magnetic effect – strong
interaction with a magnetic dipole. High dielectric constant.)
|
10 ≤ μ ≤
250
Ferrites are a class of ceramic materials that are good insulators,
high mu, 10< eps <15, specific resistivities E14 greater than
metals.
Magnetically lossy accounted for with a complex
permeability.
|
Ferrites in addition have low conductivities, i.e. large resistance. Thus,
they have low losses in the face of alternating current and produce isolators,
hybrids, gyrators and phase shifters. “Ferrites have their magnetic
ions distributed over at last two interpenetrating sublattices. A sublattice
has magnetic moments aligned but sublattices are oppositely
directed.” [2517]
|
Noting or pertaining to a substance, as a ferrite, in which the magnetic
moments of some neighboring atoms point in opposite directions, with a net
magnetization still resulting because of differences in magnitudes of the
opposite moments.
Ferrite have non-reciprocal properties including different phase constants
and phase velocities for right vs. left-hand circularly polarized waves,
different transmission coefficients as a function of direction of travel,
permeabilities that are tensors.
|
|
Ferromagnetic
|
250 ≤ μ ≤
1,000,000
High conductivity and thus cannot hold a field. Thus, they
serve to zero out electromagnetic fields.
Magnetically lossy accounted
for with a complex permeability.
|
The individual atoms in the absence of an applied magnetic field still
possess very strong magnetic moments from uncompensated electron spin moments.
After applying a Magnetic field, domains, groups of atoms with the
magnetic moment in the same direction, line up and this creates a residual
magnetic field or Magnet even when removing the external magnetic
field. [2518]
|
Noting or pertaining to a substance, as iron, that below a certain
temperature, the Curie point, can possess magnetization in the absence of an
external magnetic field; noting or pertaining to a substance in which the
magnetic moments of the atoms are aligned.
|
29.2.4 Wave Equations
The propagation constant equals the attenuation constant plus the phase
constant:
γ =
α +
jβ
Phase velocity is:
vp =
ω/β
Beta is the phase constant, phase number, or wave number and is in
radians/meter. Also
β =
2π/λ
Beta is the number of waves there are in a meter multiplied by
2π. Hence, Beta is directly
proportional to frequency since:
λ = c/f
β =
f *
2π/c
β = ω/2π *
2π/c
β = ω /
c
where ‘c’ is the speed of light. If we are not in free space
than we replace ‘c’ with ‘vp’ and end up with
a form of the equation of phase velocity above.
29.3 Computer
Networking
29.3.1 Standards
We can breakdown communication into five layers of operation from higher
logical layers to lower physical implementations. These are the OSI standard
Layers.
Table
29-6: Internet Protocol Stack
|
Layer
|
IP Stack
|
Protocol Stack or Data Unit (PDU)
|
|
5
|
Application – HTTP – web support SMTP - email
support FTP – file transfer
|
Message – This is can be an IPC – inter process communication
message.
|
|
4
|
Transport TCP UDP
|
Segment
|
|
3
|
Network IP – Internet Protocol
|
Datagram Source Routing Virtual circuits
|
|
2
|
Link – routing layer Ethernet ATM Frame
Relay PPP – modem communication
|
Frame Collisions and backoff
|
|
1
|
Physical Twisted pair copper Co-axial cable Fiber
optic
|
PDU1 – Each Layer 2 Link may have a different protocol for
transmitting bits over the different mediums.
|
29.3.2 Link
29.3.2.1 Ethernet
Ethernet operates at Layer 2 and its main feature is that it shares the
physical network by supporting collision sense and multiple access and collision
avoidance (CSMA/CA).
29.3.2.2 ATM
ATM provides protocols from the transport layer down through the physical
layer. ATM sends data in
cells of 53 bytes in length. Each cell has a 5
byte header and a 48 byte
payload. Fixed length cells and simple
headers facilitate high speed
switching.
[2519] ATM supports
virtual channels through its cell header
virtual channel identifier
(VCI). Packet switches or routers read the VCI and route cells towards the
destination. ATM runs over any physical layer achieving speeds of 600 Mps over
fiber optics. TCP/IP is operating over 100 Mbps Ethernet and holds a standard
position in the PC and LAN arena. IP over ATM operates by a router first
processing the IP header and then using the ATM ARP table to process and send
the ATM data.
Asynchronous Transfer Mode provides
network-assisted
congestion control. In essence as a cell of data travels from source to
destination, switches along the pathway add information to Resource Management
cells denoting on the congestion level. Either the switch or the destination
will return the RM cell back to its source. The source in turn will process the
RM cell to adjust the maximum rate at which to send data. The source
intersperses RM cells amongst Data cells.
Each data cell contains an
EFCI (explicit forward, congestion indication) bit. If a
switch sets the
EFCI bit in a data cell then the destination knows that it must return
congestion information to the sender. Consequently, the destination will set
the CI (congestion indication) in the subsequent RM cell before returning the
cell to the sender.
An RM cell also contains the NI (no increase) bit
that a switch may set in a passing RM cell to indicate mild congestion. The
switch may set the CI bit on more severe congestion. The destination may
return the RM cell intact, or adjust the CI bit itself based on an EFCI from a
preceding data cell. Each RM cell also contains a two-byte ER (explicit rate)
field. As the RM cells passes from source to destination, the congested switch
may only lower ER to the rate of itself. In this manner, the ER field will
contain the minimal rate of the entire path when the RM cell is returned to the
source.
[2520]
29.3.3 Network
The IP Layer 3 defines Internet communication.
29.3.4 Transport
29.3.4.1 TCP/IP
TCP/IP provides end-end congestion control. TCP – Telnet
Communication Protocol provides interactive communication. IP – Internet
Protocol provides reliable data transfer.
29.4 Satellite
Theory
29.4.1 SATCOM
SATCOM – satellite communications applies astronomy, communication
theory, and electrical engineering in the development of satellite technology.
Uplink frequencies use the higher frequency of the bands while download is of
lower frequency. Higher frequency transmission requires more power as the
quanta of energy is proportional to frequency. One advantage is that a smaller
satellite dish is sufficient to capture a signal at a higher frequency. Newer
satellite TV systems transmit at higher frequencies and customers consequently
get by with smaller dishes on their roofs.
Table
29-7: SATCOM Frequencies
|
Frequency Range in GHz
|
Frequency Band
|
Usage
|
|
0.1-0.3 (100-300 MHz)
|
VHF
|
Basic TV transmission
|
|
0.3-1.0 (300-1000 MHz)
|
UHF
|
Extended TV transmission
|
|
1.0-2.0
|
L
|
|
|
2.0-4.0
|
S
|
|
|
4.0-8.0
|
C
|
FSS – fixed satellite services. These included original cable
transmission to centers for distributing cable TV. Later these signals were
encrypted to prevent pirating FSS channels with large satellite
dishes.
|
|
8.0-12.0
|
X
|
|
|
12.0-18.0 Downlink 12.2 – 12.7 Uplink 17.3 –
17.8
Downlink 11.7 – 12.2 Uplink 14 –
14.5
|
Ku – High Power BSS – broadcast satellite service
DBS – direct broadcast satellite Point to point allowed too.
No adjacent satellite interference Ku – Medium Power FSS –
fixed satellite service Point to point primary use DBS allowed
too. Adjacent satellite interference
|
Covers broadcast satellite TV No terrestrial interference. 9 degree
spacing – ITU reg. EIRP (equivalent isotropic radiated power) –
51-60 dBW
2 degree spacing – FCC regulated. EIRP –
40-48 dBW
|
|
18.0-27.0
|
K
|
|
|
27.0-40.0
|
Ka
|
|
|
40.0-75
|
V
|
|
|
75-110
|
W
|
|
|
110-300
|
mm
|
This would be millimeter-wave which occurs in guided missile
communication.
|
|
300-3000
|
μm
|
|
INTELSAT – International Telecommunications Satellite regulates
international satellite location and operation assignments. Individual
countries on the other hand operate Domsats – Domestic satellites for
services such as voice, data, or video conferencing within a country. Domsats
are in geostationary orbit so they have a constant position over a particular
country. There is only one geostationary orbit for the world and that is over
the equator. Satellites operate at 36,000 km in this functional area.
In contrast to the singular geostationary orbit, there are an infinite
number of polar orbits. Weather satellites operate in polar orbits, usually at
altitudes of 800 and 900 km. NOAA operates both geostationary operational
environment satellites, GOES, and polar operational environment
satellites, POES. The polar orbiting satellites are sun
synchronous, i.e. crossing the equator at the same local time each day.
There are two polar satellites in orbit at a time.
Table
29-8: Polar Orbiting Satellites
|
POES Satellite
|
Height
|
Direction
|
TOD crossing equator
|
|
Morning orbit
|
830 km
|
south to north
|
7:30 AM
|
|
Afternoon orbit
|
870 km
|
south to north
|
1:40 PM
|
NOAA satellites participate in
search and rescue, SAR operation.
Russian satellites support this network with
Cospas. NOAA satellites
operate with
Sarsat.
[2521]
Originally, SAR operated only with satellites in low earth orbits, LEOs,
supporting the system LEOSAR. Recently, NOAA added geostationary satellites to
their services, which constitute GEOSAR.
When a vehicle becomes lost, its
emergency beacon transmits a signal in the VHF/UHF range at a precise frequency.
The velocity of the satellite relative to the beacon enables the satellite to
measure the Doppler shift. As a POES satellite nears the latitude of a lost
craft’s beacon, the received frequency is higher than the transmitted
frequency. As it recedes from the beacon, the received frequency is smaller
than the transmitted frequency. In this manner the POES determines the latitude
position. On the second pass, the change in the earth’s rotation permits
the satellite to determine the effect of rotation on the Doppler shift and to
identify a precise longitude position.
Sarsat’s downlink frequency
is 1544.5 MHz. to local user terminals, LUTs. The higher frequency alleviated
the false alerts caused by interference from the older emergency locator
transmitters, ELTs, operating at 121.5 MHz. There are about 600,000 distress
beacons on aircraft and small vessels.
Table
29-9: Emergency Locator Transmitters
|
System
|
ELT Frequency
|
False Alerts
|
Operation
|
Power
|
Positional Accuracy
|
|
Compas-Sarsat
|
121.5 MHz
|
98%
|
LEOSAR, polar orbit, Doppler shift, no identification info.
|
a few tenths of a watt
|
10-20 km
|
|
New Compas-Sarsat
|
406.028 MHz
|
Changed from 406 MHz to avoid conflict with GEOSTAR
|
LEOSAR,
|
5 watts
|
3-5 km
|
|
GEOSAR
|
406 MHz
|
|
Stationary orbit, GPS operation, no Doppler shift from stationary
orbits.
|
|
|
29.5 Frequency
Allocations for Broadcasting
Radio signals are vertically polarized while TV signals are
horizontally polarized.
Table
29-10: Frequency Allocations for
Broadcasting
|
Band
|
Frequency Range
|
Good Antenna Length
|
Description
|
|
AM
|
535-1605 KHz
|
140 m. – 47 m.
|
~107 channels: Interchannel Spacing 10 KHz
|
|
FM
|
88-108 MHz
|
0.85 m. – 0.69 m.
|
100 channels each 200 KHz wide
|
|
SW (international)
|
5.95 – 26.1 MHz
|
12.6 m. – 2.9 m.
|
|
29.6 Microwave
Engineering
29.6.1 Skin Depth
Skin depth of microwave frequency radiation is dependent on the
conductivity of skin which varies with frequency.
Equation
29-5: Skin depth of Radiation
δs = sqrt
(1/(f
*
π*
μ0*
σ))
where
σ is the conductivity of
the material.
μ0 is
mobility in free space
4
πe-7.
For sea water
σ = 4 siemens/meter at 10 GHz
gives
δs = 0.002515
meters or ~ 2 mm.
The conductivity of skin varies over frequency so
σ ≈ 1:10 siemens/meter from
1:10 GHz.
[2522]A microwave
oven works at 2.45 GHz.
Figure
29-3: Radiation penetration of skin vs.
Frequency
29.6.2 Fault Detection in a Cable
The Reflection coefficient is negative for a short circuit type of fault or
positive if the fault is of an open circuit type from the following analysis.
ZL is the load resistance that is 0 for a short circuit or infinity
for an open circuit. Z0 is the intrinsic impedance.
29.7 Test
Engineering
Isolating problems in test engineering is similar to being a detective.
These axioms apply:
Text
29-1: Arthur Conan Doyle—Sherlock Holmes on
Deduction
If you eliminate the impossible, whatever remains, however improbable,
must be the truth.
There should be no combination of events for which the wit of man cannot
conceive an explanation.
When all other contingencies fail, whatever remains, however improbable,
must be the truth.
Very effective my dear Watson. --Elementary my dear Holmes,
Elementary.[2523]
29.8 House
29.8.1 Lowering the Thermostat to Save
Energy
At night, one can lower the thermostat to a minimum of 55 degrees. For
each degree reduction for an eight-hour period, one can save 1% on heating
costs.
[2524] For example, for a
5-degree reduction for 16 hours, one can save 10% on the monthly heating bill
and even more if the heating rates are progressive. Pipe freezing may occur if
the house is set to 50 degrees so there is a 5-degree margin here. “If
you're away from home during winter, set the thermostat in your house to no
lower than 55 degrees to prevent pipes from freezing during a cold snap while
you're away. Open cabinet doors to allow heat to get to uninsulated pipes under
sinks and appliances near exterior
walls.”
[2525]
“For winter operation, consider setting the thermostat to 55
degrees at night when you sleep and at 68 degrees when you're home. (
In
colder parts of California,
it's not recommended to set the temperature
below 50 degrees, because indoor water pipes may freeze.)
For summer
operation, set the temperature to 78 degrees when you're home and at 85 degrees
or higher when the house is unoccupied. In the summer season, you might need to
program your thermostat to cool only for one period of the day, such as the late
afternoon and evening hours, when the family returns
home.”
[2526]
29.9 Place
Holder
[2498] Advanced Engineering
Electromagnetics, Balanis,
p.5.
[2499] Advanced
Engineering Electromagnetics, Constantine Balanis,
p.6
[2500] Fields and Waves
in Communication Engineering, Ramo,
p.13
[2501] AEE,
p.59
[2502] AEE,
p.44
[2503] AEE, Balanis,
p.60
[2504] AEE, Balanis,
p.3
[2505] AEE,
p.80
[2506] AEE,
pp.53-54
[2507] AEE, Balanis,
Fig.2-9.p.54.
[2508] AEE
p.45
[2509] Random House
Dictionary
[2510] AEE,
Balanis, pp.7-8
[2511] AEE,
Balanis, p.71
[2512] Ibid,
p.71
[2513] AEE, Balanis
p.56
[2514] Classical
Electromagnetic Radiation 3
rd Edition, Heald and Marion, 1995,
p.23
[2515]
Ibid
[2516] Classical
Electromagnetic Radiation 3
rd Edition, Heald and Marion, 1995,
p.24
[2517] AEE, Balanis
p.85
[2518] Advanced
Engineering Electromagnetics, Balanis
p.58
[2519] Computer
Networking, Kurose and Ross, p
57.
[2520] Computer
Networking
A Top-Down Approach Featuring the Internet,
James Kurose and Keith
Ross.
[2521] Sarsat refers to
locating equipment on the
satellite.
[2522] http://ej.iop.org/links/q47/cAkVjWiQU1Qf9fZG,l18cA/m10603.pdf
Changes in the dielectric properties of rat tissue as a function of age at
microwave frequencies
http://www.telecomlab.gr/2002/oct/rhodes/pap3rs/N%20123%20(p875%20-%20p881).pdf
Heat Effect Analysis of Microwave Exposed Skin by Using a Multilayer Human Skin
Model
[2523] When Sherlock
tries to determine a frequency for repelling flies and Watson resorts to the fly
swatter.
[2524] http://www.utah.gov/governor/docs/Energy_Conservation_Tips.pdf
[2525] http://www.statefarm.com/sflocal/sunland/sun_hm.htm
[2526] http://www.consumerenergycenter.org/homeandwork/homes/inside/heatandcool/thermostats.html