electrical theory for dummies
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- In electronic or electrical circuits: electrons (and charged ions, both positive and negative)
- In pneumatic circuits: compressed gas (normally ordinary air)
- In hydraulic circuits: pressurized, relatively incompressible fluid
Parts of a circuit
Every circuit consists of three basic components:
- "Active components": Source of energy
- Transmission lines
- Control devices (optional)
- "Passive components": Load
A gun, a rocket and an internal combustion engine all use compressed gas to do work, but the spent gas is vented to the atmosphere and is not reused in the system, so these are not examples of pneumatic circuits. Refrigeration systems do, however, recycle the compressed gases they use, but are not typically thought of as circuits.
Circuit vs. network
An electrical circuit is a collection of electrical components which accomplish a specific task such as heating, lighting or running a motor. This collection may or may not form a complete topological loop, depending on whether it is presently connected to power, integrated into a larger device or circuit, or damaged. Sometimes, it is convenient to speak of an electrical circuit as a network, de-emphasizing the return path. Return paths are sometimes omitted from circuit diagrams, making the resulting graphic visually resemble a network topology rather than some sort of loop topology. See circuit diagram and schematic.
Open circuit vs. closed circuit
A fundamental part of circuit analysis is determining whether the matter has a return path to the power source. If the matter is blocked from returning to the power source, either wholly or partially, the entire assemblage will be prevented from accomplishing work. In an electrical circuit, an open circuit is caused intentionally when a user opens a switch or unintentionally when vibration or mechanical damage severs a wire. In a pneumatic or hydraulic circuit, this occurs when a valve is closed or there is a leak in one of the lines or components.
In electrical circuits, closing a switch creates a closed loop for the electrons to flow through. This is sometimes referred to as "completing the circuit."
In an electrical or electronic circuit, sometimes an unintended connection is made, such as when insulation is broken, frayed, melted or chewed by rodents, or a technician inserts a metal tool into a live device. When this happens, current bypasses some or all of the components in the circuit, taking a "shorter" path back to the power source. This can lead to excessive current drain, which in turn generates excessive heat, damaging or destroying sensitive parts of the system such as transistors and ICs.
In Graph theory, an edge whose two ends meet is called a loop, which is an entirely different usage of the word. In any kind of circuit, such a loop has no distinct function. An argument can be made that redundant lines for transmission of power do have a function, even if it is only a backup function.
There are three basic types of circuit currently used in industry:
The following is a rough list of the types of components which make up each type of circuit.
- Sources of energy
- Sources of energy
- Transmission lines
- Air tank
- Pneumatic hoses
- Open atmosphere (for returning the spent gas to the compressor)
- Passive components
In physics, a unified field theory (occasionally referred to as a "uniform" field theory) is a type of field theory that allows all that is usually thought of as fundamental forces and elementary particles to be written in terms of a single field. There is no accepted unified field theory. It remains an open line of research. The term was coined by Einstein, who attempted to unify the general theory of relativity with electromagnetism, hoping to recover an approximation for quantum theory. A "theory of everything" is closely related to unified field theory, but differs by not requiring the basis of nature to be fields, and also attempts to explain all physical constants of nature.
This article describes unified field theory as it is currently understood in connection with quantum theory. Earlier attempts based on classical physics are described in the article on classical unified field theories.
There may be no a priori reason why the correct description of nature has to be a unified field theory; however, this goal has led to a great deal of progress in modern theoretical physics and continues to motivate research. Unified field theory is only one possible approach to unification of physics.
According to the current understanding of physics, forces between objects (e.g. gravitation) are not transmitted directly between the two objects, but instead go through intermediary entities called fields. All four of the known fundamental forces are mediated by fields, which in the Standard Model of particle physics result from exchange of bosons (integer-spin particles). Specifically the four interactions to be unified are (from strongest to weakest):
- Strong interaction: the interaction responsible for holding quarks together to form neutrons and protons, and holding neutrons and protons together to form nuclei. The exchange particle that mediates this force is the gluon.
- Electromagnetic interaction: the familiar interaction that acts on electrically charged particles. The photon is the exchange particle for this force.
- Weak interaction: a repulsive short-range interaction responsible for some forms of radioactivity, that acts on electrons, neutrinos, and quarks. It is governed by the W and Z bosons.
- Gravitational interaction: a long-range attractive interaction that acts on all particles with mass. The postulated exchange particle has been named the graviton.
Modern unified field theory attempts to bring these four force-mediating fields together into a single framework. Quantum theory seems to limit any deterministic theory's descriptive power (in simple terms, no theory can predict events more accurately than allowed by the Planck constant).
The first successful (classical) unified field theory was developed by James Clerk Maxwell. In 1820 Hans Christian Ã˜rsted discovered that electric currents exerted forces on magnets, while in 1831, Michael Faraday made the observation that time-varying magnetic fields could induce electric currents. Until then, electricity and magnetism had been thought of as unrelated phenomena. In 1864, Maxwell published his famous paper on a dynamical theory of the electromagnetic field. This was the first example of a theory that was able to encompass previous separate field theories (namely electricity and magnetism) to provide a unifying theory of electromagnetism. Later, in his theory of special relativity, Albert Einstein was able to explain the unity of electricity and magnetism as a consequence of the unification of space and time into an entity we now call spacetime.
In 1921 Theodor Kaluza extended General Relativity to five dimensions and in 1926 Oscar Klein proposed that the fourth spatial dimension be curled up (or compactified) into a small, unobserved circle. This was dubbed Kaluza-Klein theory. It was quickly noticed that this extra spatial direction gave rise to an additional force similar to electricity and magnetism. This was pursued as the basis for some of Albert Einstein's later unsuccessful attempts at a unified fi
An electrical network is an interconnection of electrical elements such as resistors, inductors, capacitors, transmission lines, voltage sources, current sources and switches. An electrical circuit is a special type of network, one that has a closed loop giving a return path for the current. Electrical networks that consist only of sources (voltage or current), linear lumped elements (resistors, capacitors, inductors), and linear distributed elements (transmission lines) can be analyzed by algebraic and transform methods to determine DC response, AC response, and transient response.
To design any electrical circuit, either analog or digital, electrical engineers need to be able to predict the voltages and currents at all places within the circuit. Linear circuits, that is, circuits with the same input and output frequency, can be analyzed by hand using complex number theory. Other circuits can only be analyzed with specialized software programs or estimation techniques such as the piecewise-linear model.
A number of electrical laws apply to all electrical networks. These include:
- Kirchhoff's current law: The sum of all currents entering a node is equal to the sum of all currents leaving the node.
- Kirchhoff's voltage law: The directed sum of the electrical potential differences around a loop must be zero.
- Ohm's law: The voltage across a resistor is equal to the product of the resistance and the current flowing through it (at constant temperature).
- Norton's theorem: Any network of voltage and/or current sources and resistors is electrically equivalent to an ideal current source in parallel with a single resistor.
- ThÃ©venin's theorem: Any network of voltage and/or current sources and resistors is electrically equivalent to a single voltage source in series with a single resistor.
- See also Analysis of resistive circuits.
Other more complex laws may be needed if the network contains nonlinear or reactive components. Non-linear self-regenerative heterodyning systems can be approximated. Applying these laws results in a set of simultaneous equations that can be solved either by hand or by a computer.
Network simulation software
Linearization around operating point
When faced with a new circuit, the software first tries to find a steady state solution, that is, one where all nodes conform to Kirchhoff's Current Law and the voltages across and through each element of the circuit conform to the voltage/current equations governing that element.
Once the steady state solution is found, the operating points of each element in the circuit are known. For a small signal analysis, every non-linear element can be linearized around its operation point to obtain the small-signal estimate of the voltages and currents. This is an application of Ohm's Law. The resulting linear circuit matrix can be solved with Gaussian elimination.
Software such as the PLECS interface to Simulink uses piecewise-linear approximation of the equations governing the elements of a circuit. The circuit is treated as a completely linear network of ideal diodes. Every time a diode switches from on to off or vice versa, the configuration of the linear network changes. Adding more detail to the approximation of equations increases the accuracy of the simulation, but also increases its running time.
From Yahoo Answers
Answers:For any wave, like a sound wave, light wave, AC electric wave, ocean wave any wave at all, you can define three properties, the frequency of the wave, the wavelength of the wave and the velocity of the wave. The freqency is simply how many oscillations is makes in one second. So say you had a pendulum swinging back and forth. If It starts at one side, swings to the other and back 5 times every second, then the frequency is 5Hz (1Hz is one cycle per second). If it swings back and forth 7 times every 5 seconds, then the frequency is 7 cycles per 5 seconds, which is 7/5 Hz which is 1.4 Hz. Same can be applied to an AC electric current, if it starts at 0, goes to some positive value, then to a negative value, then back to zero this is one cycle. If it makes 5 cycles every second this is 5 Hz. The period of a wave is how long (in seconds) does it take to complete one cycle. So if you have a wave that is 5Hz in frequency, this means it completes 5 cycles every second. So it takes one fith of a second to complete one cycle. So we say the period is 1/5 seconds. Like wise, say the wave makes 11 cycles in 4 seconds. Then its frequency is 11/4 Hz. So this means it makes 11/4 cycles in one second. So it takes 4/11 seconds to make one cycle, so the period is 11/4. In general, you may have noticed that the period is equal to one over the frequency: T=1/f The velocity or speed of a wave is how rapidly does one 'feature' of a wave move though the medium. So if you go to the beach or a river and watch water waves, if you look at one crest, you can see it appears to move along the surface. The speed of the wave is how fast this crest (or any other part of the wave for that matter) moves along. For electromagnetic waves, this is the speed of light when in a vacuum or air, and for electromagnetic waves along a wire, it is usually some fraction of the speed of light. The wave length of a wave is the physical distance between one peak and the next (or one trough and the next, or any other part of the wave and the next one for that matter). If you can imagine you freeze time and look at the wave, you could get a ruler out and measure this. But you can of course not do this. Instead, notice there is a relation between the wavelenght, the speed of the wave, and the frequency (or period.) Say for example the wave moves at one meter per second, and you know the frequency is one hertz. Then by the time the wave has moved along one meter, it has gone through one complete cycle: the wave lenght must be one meter. Another exampl, say once again the wave is traveling at 1m/s and now its frequency is 2Hz. Now it completes 2 cycles every meter, so each cycle must be 1/2 a meter long. Its wavelength is 1/2 a meter. So the general relation between wave lenght and frequency and speed is: L=c/f where L is the wave length, c is the speed of the wave, and f is the frequency. You can also write this in terms of the period T of the wave: L=c*T Now we are ready to do the questions! 1) the wave has a period of 1/1000 seconds. This means it completes 1000 cycles in one second, so its frequency is 1000Hz 2) From our above explaination, we know that the period T is 1/f, so for 1MHz, this is 1/1000000 or in other words, 1 micro second, and for 2MHz, this is 1/2000000, which is half a microsecond 3) The wavelength as we know can be found from the relation =c/f we know the f=30GHZ, but whats the speed? Well it is a radio wave, so its speed (assuming it is traveling through air or a vacuum), is the speed of light, which is 3x10^8 m/s so we can now calculate the wavelenght: = 3x10^8/(30x10^9) m = 1/10 x 10^-1 m = 1 cm I think you should be able to do the rest now! (for question 5 and 6, remember the speed of sound at sea level and 1atm of pressure and 0 degrees celcius is about 344 meters per second!)