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Amplitude Modulation An AF voice signal has frequencies mostly in the range between 300 Hz and 3 kHz Some characteristic of an RF carrier can be varied, or modulated, by these waveforms, thereby transmitting voice information Figure 25-2 shows a simple circuit for obtaining amplitude modulation (AM) This circuit can be imagined as an RF amplifier for the carrier, with the instantaneous gain dependent on the instantaneous audio input amplitude Another way to think of this circuit is as a mixer that combines the RF carrier and audio signals to produce sum and difference signals at frequencies just above and below that of the carrier The circuit shown in Fig 25-2 works well, provided the AF input amplitude is not too great If the AF input is excessive, then distortion occurs, intelligibility is degraded, system efficiency is reduced, and the bandwidth of the signal is increased unnecessarily The extent of AM is expressed as a percentage, from 0 percent (an unmodulated carrier) to 100 percent (full modulation) Increasing the modulation past 100 percent causes the same problems as excessive AF input In an AM signal modulated 100 percent, 1 3 of the power is used to convey the data, and the other 2 3 is consumed by the carrier wave Figure 25-3 shows a spectral display of an AM voice radio signal The horizontal scale is calibrated in increments of 1 kHz per division Each vertical division represents 3 dB of change in signal strength The maximum (reference) amplitude is 0 dB relative to 1 mW (abbreviated as 0 dBm) The data exists in sidebands above and below the carrier frequency These sidebands resemble the sum and difference signals produced by a mixer In this case the mixing occurs between the AF input signal and the RF carrier The RF between 3 kHz and the carrier frequency constitutes the lower.

The accelerometer error state vector xa discussed below has dimension thirty In fact, the potential state order could be higher depending on the dynamic model that is appropriate for each state element (eg, random constant, scalar Gauss-Markov) In any particular application, the entire vector xa may not be required; instead, the designer must determine which error terms have a signi cant e ect on performance Those terms must be identi ed either in the laboratory or during on-line operation Bias Error (3 States) De ne the bias as xba = ba The e ect of the bias error on the speci c force error is f p = I xba (11119)

Scale Factor and Misalignment (9 States) Aa = SFa a which has the form p SFu Aa = avw awv auw SFv awu

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sideband (LSB); the RF from the carrier frequency to +3 kHz represents the upper sideband (USB) The bandwidth is the difference between the maximum and minimum sideband frequencies, in this case 6 kHz In an AM signal, the bandwidth is twice the highest audio modulating frequency In the example of Fig 25-3, all the voice energy is at or below 3 kHz, so the signal bandwidth is 6 kHz This is typical of a communications signal In standard AM broadcasting, the AF energy is spread over a wider bandwidth, nominally 10 kHz

(11120)

Single Sideband In AM, most of the RF signal power is consumed by the carrier alone; the two sidebands are mirrorimage duplicates This is inefficient, and is also unnecessarily redundant! If the carrier and one of the sidebands is eliminated, these shortcomings can be overcome That makes the signal stronger for a given amount of RF power, or allows the use of lower RF power in a given communications scenario Another bonus is the fact that the bandwidth is reduced to less than half that of an AM signal modulated with the same data, so more than twice as many signals can fit into a specific range, or band, of frequencies When the carrier is removed from an AM signal along with one of the sidebands, the remaining RF energy has a spectral display resembling Fig 25-4 This is single sideband (SSB) transmission Either the LSB or the USB alone can be used, with equally good results

De ne the auxiliary state composed of the accelerometer scale factor and misalignment matrix parameters to be xAa = [SFu , SFv , SFw , auw , auv , avw , avu , awv , awu ] The partial derivative of fu f p = 0 xAa 0 f p with respect to xAa is 0 fv 0 0 0 fw fv 0 0 fw 0 0 0 fu 0 0 fw 0 0 0 fu 0 0 fv (11121)

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