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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
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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

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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.

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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.

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Equation ‎29-3: Ampere's Law
Ampere’s law for statics is x H = J. Maxwell added the electric displacement current density J= ∂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:

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:
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.
Jd = ∂D/∂t = jωD = jωεE
that is the change in the Electric Flux Density[2505] in C/(s-m2)
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] 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 4πe-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
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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.

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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 3rd Edition, Heald and Marion, 1995, p.23
[2515] Ibid
[2516] Classical Electromagnetic Radiation 3rd 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

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