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The hydrocarbon fraction consists of methane to high-boiling tar The composition of this fraction can be influenced by many parameters, such as particle size of the biomass, temperature, pressure, heating rate, residence time, and catalysts The operative reactions are: C + CO2 2CO C + H2O H2 + CO 2C + 2H2O 2H2 + CO2 + CO C + 2H2 CH4 CO + H2O CO2 + H2 CO + 3H2 CH4 + H2O The composition of the producer gases varies widely with the properties of the biomass, the gasifying agent, and the process conditions Depending on the nature of the raw solid feedstock and the process conditions, the char formed from pyrolysis contains 20 to 60 percent of the energy input.

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Therefore, if the delta pseudorange is divided by T it measures the average rate of change of the pseudorange over the indicate time interval. By the mean value theorem, there is a value of q [ r (t) T, r (t)] such that s (q) = 1 ( r (t)). By this reasoning the delta pseudorange observable is r T often modeled as the rate of change of the pseudorange at the midpoint of the interval r [ r (t) T, r (t)] and referred to as the Doppler observable. The validity of this modeling assumption depends on the bandwidth of the vehicle B relative to T . Eqn. (8.31) is the de nition of the delta pseudorange observable, but the observable is not constructed by di erences of the pseudorange observable. Instead, for a channel that has achieved phase lock for the carrier signal, the delta pseudorange observable is constructed from di erences of the carrier phase observable over the period T . In this case, cycle slips or loss of phase lock during the interval, if not detected, will result in erroneous observables. For a channel that has only achieved frequency lock for the carrier signal, the delta pseudorange is constructed from the channel s replica Doppler frequency. In this case, loss of frequency lock during the interval will result in erroneous observables if not detected. Assuming that the receiver has and maintains phase lock over the interval r [ r (t) T, r (t)] that is of interest, then the Doppler observable can be computed as r (t) = i ( r (t)) i ( r (t) T ) . r r (8.33)

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