With the state vector of the ith particle at
time t expressed by t i x , =(xt,i, yt,i, t ,i ), encoder travel from
time t - 1 until time t, by t v and changes in yaw angles ψ as
measured by the gyroscope by , the movement of
particles by DR are expressed by Eq. (7):
With the state vector of the ith particle attime t expressed by t i x , =(xt,i, yt,i, t ,i ), encoder travel fromtime t - 1 until time t, by t v and changes in yaw angles ψ asmeasured by the gyroscope by , the movement ofparticles by DR are expressed by Eq. (7):
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