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where x = p , c tr Therefore, the standard GPS positioning problem involves estimation of four unknown quantities: the three components of p and tr The vector x is estimated based on pseudorange measurements which for the L1 pseudorange can each be modeled as i 1 r = (x, pi ) + c ti + f2 i i i i I + Tr + M 1 + 1 f1 r (83)

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Graphic Equalizer A graphic equalizer is a device for adjusting the relative loudness of audio signals at various frequencies It allows tailoring of the amplitude versus frequency output of hi-fi sound equipment Equalizers are used in recording studios and by serious hi-fi stereo enthusiasts There are several independent gain controls, each one affecting a different part of the audible spectrum The controls are slide potentiometers with calibrated scales The slides move up and down, or, in some cases, left to right When the potentiometers are set so that the slides are all at the same level, the audio output or response is flat, meaning that no particular range is amplified or attenuated with respect to the whole AF spectrum By moving any one of the controls, the user can adjust the gain within a

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where c is the speed of light, f1 is the L1 carrier frequency, and f2 is the L2 carrier frequency The subscript r on refers to the receiver Later in the chapter, when multiple receivers are considered, the subscript r will be used to count over the available receivers The subsubscript 1 refers the measurement to the L1 signal Using the same notational conventions, the L2 pseudorange can be modeled as i 2 r = (x, pi ) + c ti + f1 i i i i I + Tr + M 2 + 2 f2 r (84)

The error models of eqns (83 84) are derived in Section 84 The measurement error components are de ned as follows:

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certain frequency range without affecting the gain outside that range The positions of the controls on the front panel provide an intuitive graph of the output or response curve Figure 31-4 is a block diagram of a hypothetical graphic equalizer with seven gain controls The input is fed to an audio splitter that breaks the signal into seven paths of equal impedance, and prevents interaction among the circuits The seven signals are fed to audio attenuators, also called bandstop filters, each filter having its own gain control (The center frequencies of the attenuators in this example are at 30, 100, 300, and 900 Hz, and 25, 7, and 18 kHz These are not standard frequencies, and are given here only for illustrative purposes) The slide potentiometers affect the extent to which each filter affects the gain within its frequency range Finally, the signals pass through an audio mixer, and the composite is sent to the output There are several challenges in the design and proper use of graphic equalizers The filter gain controls must not interact Judicious choice of filter frequencies and responses is important The filters must not introduce distortion The active devices must not generate significant audio noise Graphic equalizers are not built to handle high power, so they must be placed at low-level points in an audio amplifier chain In a multichannel circuit such as a stereo sound system, a separate graphic equalizer can be used for each channel

Section 25 de ned the Euler angles ( , , ) and described their use to determine the direction cosine matrix Rg This method of determining b

Mobile and portable hi-fi systems operate at low dc voltages Typical audio power levels are much lower than in home hi-fi systems Speakers are much smaller also In portable systems, headsets are often used in place of speakers

the direction cosine matrix requires the navigation system to measure or compute the Euler angles This section presents the method for comput ing the Euler angle derivatives ( , , ) from the angular rate vector b gb The navigation system could then integrate the Euler angle derivatives, to determine the Euler angles from which the direction cosine matrix can be computed Note that the three-tuple ( , , ) is not related to b by a rotational gb transform because each of the components of ( , , ) is de ned in a di erent reference frame Instead, we have that b = b + b + b gb g1 12 2b (271)