A typical amplifier examines the current flowing in its input circuit and produces a current in its output circuit that's proportional to but much larger than this input current. The factor by which the amplifier multiplies the input current to produce the output current is sometimes called the amplifier's "current gain." The tiny currents produced by a microphone attached to an audio amplifier's input circuit are boosted into huge currents that flow through speakers attached to the amplifier's output circuit. Since your voice is controlling these large currents, the speakers reproduce the sound of your voice.
While there are many techniques used to amplify currents, most modern audio amplifiers use transistors to do the amplification. A transistor is a device that permits a small current or electric charge to control the flow of a much larger current. The transistors inside the amplifier examine the current in the amplifier's input circuit and these transistors control the current passing through the amplifier's output circuit. Because the current in the output circuit needs electric power to continue flowing, a power supply inside the amplifier provides that current with power. As you talk into the microphone, the transistors adjust the current flowing through the output circuit so that that current is proportional to the current flowing through the input circuit.
Some audio amplifiers provide several different outputs, each characterized by the impedance of its expected load (e.g., the impedance of the speaker that you should attach to that output). This impedance measures the relationship between voltage and current that the load needs to function optimally. The higher the impedance, the more voltage the amplifier must provide to propel a particular electric current through the speaker. If the speaker that you attach to the amplifier has the wrong impedance, the amplifier won't be able to deliver its maximum audio power to the speaker and you may damage the amplifier, speaker, or both.
Since a typical household speaker has an impedance of 8 ohms, you should connect it to an amplifier's 8 ohm output. However, if you connect more than one speaker to the same output, you should be careful to determine the combined impedance. For example, two 8-ohm speakers in series have a combined impedance of 16 ohms while two 8-ohm speakers in parallel have a combined impedance of 4 ohms. Many amplifiers are designed to accommodate these arrangements.
When a distribution amplifier must send current long distances through thin wires, it will often use higher voltages and lower currents to minimize power losses in the wires. Such an amplifier expects its load to have an unusually large impedance. In this situation, the speaker that is used must either have a large impedance, so that it can use this high voltage/low current power directly, or there must be an impedance matching transformer between the amplifier and the speaker.
Electrostatic speakers uses the forces between electric charges (so called "electrostatic forces") to move a thin metal diaphragm back and forth rapidly. The motions of this diaphragm compress and rarefy the air in front of it, producing sound. On each side of the diaphragm is a rigid metallic grill that can hold electric charges. When the speaker is silent, the diaphragm has a large positive electric charge on it and both the metal grills have large negative charges on them (it could be the other way around, depending the speaker's exact design). The diaphragm is then attracted equally toward both grills and the electrostatic forces cancel perfectly. The diaphragm doesn't undergo any acceleration. To make the speaker produce sound, the electric charges on the two grills are changed so that the electrostatic forces on the diaphragm don't cancel. Instead, the diaphragm is pulled strongly toward whichever grill has more negative charge on it (or less positive charge). The charges on the grills fluctuate as the music plays and the diaphragm accelerates back and forth between the grills. It pushes on the air as it does and produces sound. You'll notice that the diaphragm is a moving part, so the claim that the speaker has "no moving parts" is misleading. The speaker cone of a conventional speaker only moves back and forth, too, so it has an equal claim to having "no moving parts." The relative expense of an electrostatic speaker comes from the requirement of careful construction and the need for a high voltage adapter to match an amplifier to the speaker.
The same touch sensors that are used in "touch" lamps or some elevator buttons could be used to sense when you touch a car. A car is essentially insulated from the ground by its rubber wheels, so that when you touch it there is a tendency for electric charge to be transferred between the earth and the car through you. That's why you may receive a shock when you touch a car on a cold winter day. Many electronic devices are capable of detecting this charge transfer (in fact, many of them would be damaged by such sudden and large charge transfers). So building a car touch sensor would be easy. Whether there is a commercial product that does this is another matter, and I am not sure of the answer.
Yes. I wouldn't try to detect mechanical contact, because you'd have trouble differentiating between forces exerted on the car by a hand and those exerted on it by sound waves. But you can tell whether a conducting object (such as a person) is near the car by looking at the car's electric properties. If you were to send electric charge on and off the car rapidly with a source of high-frequency alternating current, you would find that the amount of charge that flowed on or off the car during each cycle would change as the person's hand approached the car. That's because the charges on the car would push or pull on charges in the person's hand and the charges in the person's hand would move. In effect, the person's hand would make the car "larger" and it would draw more charge from your current source. Even if the person didn't touch the car, the nearness of the hand and car would change the way current flowed on and off the car. Such a change would be easy to detect with laboratory equipment and could probably be made by cheap consumer equipment, too. The only complications would be in not detecting everything—passing cars for example—and in not damaging the device with static discharges. Still, I think all of that could be done.
Acoustic "white noise" is a collection of random sounds that together have the same volume at every frequency or pitch. It's defined more accurately as having the same amount of power in each unit of its bandwidth, so that the acoustic power between 20 and 21 cycles per second is the same as the acoustic power between 500 and 501 cycles per second.
In analog audio, the air pressure fluctuations of sound at the microphone are represented by a continuously variable physical quantity such as an electric current, a voltage, or a magnetization. Thus as the air pressure at a tape recorder's microphone rises during one moment of a song, an electric current in the recorder will rise and a region of a magnetic tape surface will become particularly strongly magnetized in a particular direction. Overall, each value of air pressure is converted to a particular value of the physical quantity.
The problem with analog recording is that when the sound is recreated, any defect in the physical quantity representing air pressure will lead to an imperfection in the reproduced sound. For example, if the magnetization of the recording tape has changed slightly due to how it was stored, the sound that the tape recorder produces won't be exactly the same as the sound that the microphone heard. Digital recording avoids this problem by recording the information as bits. The physical quantity such as magnetization is representing bits (which take only two possible values) rather than the air pressure itself (which can take a broad range of values). Minor changes in the physical quantity representing these bits won't change the bits. Thus imperfections in the recording or playback process won't affect the sound quality.
The answer depends a little on which type of transistor is used, so I'll consider only an audio amplifier based on MOSFETs (Metal-Oxide-Semiconductor Field Effect Transistors). One of these three-electrode devices allows a tiny electric charge on its gate electrode to control a substantial current flowing between its source and drain electrodes. In a typical amplifier, the current flowing in the input circuit is allowed to deposit or remove electric charge from the gate electrode(s) of one or more MOSFETs. This action dramatically changes how much current flows in a second circuit. This second circuit is ultimately responsible for the current that passes out of the amplifier and through the speakers that reproduce sound. As the current in the input circuit fluctuates to represent a particular musical passage, the charges on the gates of the MOSFETs also fluctuate and the MOSFETs vary the current through the output circuit and the speakers. Because MOSFETs are so sensitive to even a tiny amount of charge, it doesn't take much current in the input circuit to cause large changes in the current of the output circuit.
While some modern car horns are actually specialized computer audio systems, the old-fashioned electromagnetic car horns are still common. An electromagnetic horn uses an electromagnet to attract a steel diaphragm and turns that electromagnet on and off rhythmically so that the diaphragm vibrates. In fact, it uses the diaphragm's position to control the power to the electromagnet. Whenever the diaphragm is in its resting position or even farther from the electromagnet, a switch closes to deliver electric current to the electromagnet. The electromagnet then attracts the diaphragm's center. But when the diaphragm moves closer to the electromagnet, as the result of this attraction, the switch opens and current stops flowing to the electromagnet. Because of this arrangement, the diaphragm moves in and out and turns the electromagnet off and on as it does. The diaphragm's tone is determined by the natural resonances of its surface.
My understanding is that a Zobel network consists of a resistor in series with a capacitor and that the capacitor is normally connected to ground. When you attach the free end of this network to a wire carrying an audio signal, the network acts like a frequency-dependent load. At very low frequencies, the capacitor has plenty of time to charge through the resistor and the network has little effect on the audio signal—it acts as though it weren't there. At very high frequencies, the capacitor has no time to charge through the resistor and behaves like a wire. As a result, the network acts as though it were just the resistor connecting the audio signal wire to ground. So the impedance of the Zobel network varies from infinite at low frequencies to become equal to the resistance of the resistor at high frequencies. The crossover between these two behaviors is related to the RC time constant. I think that Zobel networks are used in audio amplifiers to dampen out high frequency oscillations that might occur in the absence of loads at high frequencies.
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