MEMORIES OF MY POSTS
Wednesday, August 8, 2007
Fiber Optics

Fiber optics (optical fibers) are long, thin strands of very pure glass about the diameter of a human hair. They are arranged in bundles called optical cables and used to transmit light signals over long distances.

If you look closely at a single optical fiber, you will see that it has the following parts:
- Core - Thin glass center of the fiber where the light travels
- Cladding - Outer optical material surrounding the core that reflects the light back into the core
- Buffer coating - Plastic coating that protects the fiber from damage and moisture
Hundreds or thousands of these optical fibers are arranged in bundles in optical cables. The bundles are protected by the cable's outer covering, called a jacket. Optical fibers come in two types:
- Single-mode fibers
- Multi-mode fibers
Single-mode fibers have small cores (about 3.5 x 10-4 inches or 9 microns in diameter) and transmit infrared laser light (wavelength = 1,300 to 1,550 nanometers). Multi-mode fibers-3 inches or 62.5 microns in diameter) and transmit infrared light (wavelength = 850 to 1,300 nm) from light-emitting diodes (LEDs). have larger cores (about 2.5 x 10 Some optical fibers can be made from plastic. These fibers have a large core (0.04 inches or 1 mm diameter) and transmit visible red light (wavelength = 650 nm) from LEDs.
How Does an Optical Fiber Transmit Light?
Suppose you want to shine a flashlight beam down a long, straight hallway. Just point the beam straight down the hallway -- light travels in straight lines, so it is no problem. What if the hallway has a bend in it? You could place a mirror at the bend to reflect the light beam around the corner. What if the hallway is very winding with multiple bends? You might line the walls with mirrors and angle the beam so that it bounces from side-to-side all along the hallway. This is exactly what happens in an optical fiber.

Diagram of total internal reflection in an optical fiber
The light in a fiber-optic cable travels through the core (hallway) by constantly bouncing from the cladding (mirror-lined walls), a principle called total internal reflection. Because the cladding does not absorb any light from the core, the light wave can travel great distances. However, some of the light signal degrades within the fiber, mostly due to impurities in the glass. The extent that the signal degrades depends on the purity of the glass and the wavelength of the transmitted light (for example, 850 nm = 60 to 75 percent/km; 1,300 nm = 50 to 60 percent/km; 1,550 nm is greater than 50 percent/km). Some premium optical fibers show much less signal degradation -- less than 10 percent/km at 1,550 nm.
Advantages of Fiber Optics
Why are fiber-optic systems revolutionizing telecommunications? Compared to conventional metal wire (copper wire), optical fibers are: - Less expensive - Several miles of optical cable can be made cheaper than equivalent lengths of copper wire. This saves your provider (cable TV, Internet) and you money.
- Thinner - Optical fibers can be drawn to smaller diameters than copper wire.
- Higher carrying capacity - Because optical fibers are thinner than copper wires, more fibers can be bundled into a given-diameter cable than copper wires. This allows more phone lines to go over the same cable or more channels to come through the cable into your cable TV box.
- Less signal degradation - The loss of signal in optical fiber is less than in copper wire.
- Light signals - Unlike electrical signals in copper wires, light signals from one fiber do not interfere with those of other fibers in the same cable. This means clearer phone conversations or TV reception.
- Low power - Because signals in optical fibers degrade less, lower-power transmitters can be used instead of the high-voltage electrical transmitters needed for copper wires. Again, this saves your provider and you money.
- Digital signals - Optical fibers are ideally suited for carrying digital information, which is especially useful in computer networks.
- Non-flammable - Because no electricity is passed through optical fibers, there is no fire hazard.
- Lightweight - An optical cable weighs less than a comparable copper wire cable. Fiber-optic cables take up less space in the ground.
- Flexible - Because fiber optics are so flexible and can transmit and receive light, they are used in many flexible digital cameras for the following purposes:
Because of these advantages, you see fiber optics in many industries, most notably telecommunications and computer networks. For example, if you telephone Europe from the United States (or vice versa) and the signal is bounced off a communications satellite, you often hear an echo on the line. But with transatlantic fiber-optic cables, you have a direct connection with no echoes.
Steps for Ray Diagram of Concave mirrors
1. From the tip of the object, draw a line parallel to the principal axis to the mirror. Then, draw another line from the tip of the object to the mirror but this time, the line must pass through the focal point.

2. From the first incident ray, draw a line passing through the focal point (as by the one of the laws of reflection of concave mirrors). From the second incident ray, draw a line parallel to the principal axis.

3. The point where the two rays of reflection intersect is where the tip of the image is. Just draw a perpendicular line connecting the point of intersection and the principal axis. And that's how to make a ray diagram.. Easy, ayt?
Steps for Ray Diagram of Convex Mirrors
1. Draw a line parallel to the principal axis from the tip of the object to the mirror. Draw another line (that if extended, would pass through the focal point, which in this case, would be on the other side of the mirror) to the mirror. 
2. As by the two laws of reflection of convex mirrors, from the first incident ray, draw a line straight up or perpendicular to the principal axis. From the point of the second incident ray touching the mirror, draw a line parallel to the principal axis. 
3. To get an intersection, extend the rays.
4. The point of intersection is the tip of the object. Just draw a perpendicular line connecting it and the principal axis. 
Steps for Ray Diagram of Converging Lenses
1. Draw the first ray parallel to the principal axis. Draw the second ray passing through the vertex. Draw the third ray passing through the focal point in front of the mirror.
2. Based on the three laws of refraction for converging lenses, the ray of refraction for the first ray of incidence must pass through the focal point at the back of the lens, the second ray of incidence must travel a straight line and the third ray of incidence must form a ray of refraction parallel to the principal axis.
3. The point of intersection is the tip of the object. Just draw a perpendicular line connecting the point of intersection and the principal axis.
Steps For Ray Diagram of Diverging Lens
1. From the tip of the object, draw the first ray parallel to the principal axis. Draw a second ray that if extended would pass through the focal point of the back side of the mirror. Draw a third ray passing through the vertex.
2. Based on the three laws of refraction for diverging lenses, the ray of refraction for the first incident ray should be going up, tilted to the back side and if extended, would pass through the focal point of the front side of the lens. For the second ray, its ray of refraction must be parallel to the principal axis. For the third ray, it just goes like a straight line.
3. To get an intersection, jut extend the rays of refraction, that connect the intersection to the principal axis with a perpendicular line. Now, you're done with your ray diagram!
``larah3ptolemy0708 ; 7:08 PM
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ABOUT MY FAVE SUBJECT - PHYSICS .... duh...
Physics is an idea.
The idea is a simple one.
There's a whole lot of space out there. A whole lot!
And it ain't all what it seems.
"Who am I?" As if I dont know...
"Why am I here?" Bah.
Those questions mean nothing. If I could unfurl my mind enough to look fully into the face of space/time, I WOULD understand.
I would be enlightened... while solving these problems==>
LARAH'S PHYSICS ALPHABET
The Physics Alphabet
A is for Ampere, which makes quite good sense;
B is for Mag Field, and now I get tense.
C is for Speed, of light, oh so hectic;
D is for Moment, of dipoles electric.
e is a Base, our natural friend;
F is Momentum.
G is for Function, when "f" just won't fly;
h is Planck's Constant, which we often times by.
I is for Current, the charges all run;
J is for Bessel, his Function, such fun!
K is Potassium (some ChemPhys content);
L is Momentum, in an angular bent.
M is for Spin, when its subscript is "s";
N is for Number - which works, I confess!
O is the Empty Set (okay, so that's math);
P is Momentum, on a linear path.
Q is for Heat, to warm the cold night;
R is the Gas Constant, which I never get right.
S is for Entropy, its value we need;
T is for Energy, of the kinetic breed.
U is more Energy, potential this time;
V's also potential... NEED HELP! I can't think of a rhyme!
W is for Tungsten (one last ChemPhys fling);
X is for, well, just about Physics anything!
Y is for Functions of Bessel's second kind;
Z is for Charge, bringing up the behind.
So next time the artsies are on your back,
Critiquing your spelling in a vicious attack,
Say to them simply, looking straight in their eyes,
"I'm using my PERSONAL PHYSICS ALPHABET - what's wrong with you guys?!?"
It ain't your typical alphabet system or make not sense.
But it's MINE and for my own consumption.