Consider a local-level state-space model , , with mutually independent centered Gaussian noises of variances and . Start with , independently of these noises. Before the first observation, the Kalman prediction step gives , . If , the Kalman gain is , and the posterior mean and posterior variance become
The next Kalman prediction step keeps the mean but adds fresh process noise variance, giving . If , then
Thus new uncertainty is introduced at each transition and reduced by each measurement. It does not shrink to zero merely because many measurements have arrived: the state continues to change.
Figure 1.
A Kalman filter follows a changing scalar state and retains uncertainty about each new transition
. Top: one seeded synthetic random walk, its noisy observations and the filtered posterior mean, starting from with , . The shaded region is the mean plus or minus two posterior standard deviations, a pointwise conditional band under the stated model. Bottom: the Kalman gain approaches its positive steady value. Setting instead asserts a constant state and eventually stops adapting appreciably. This single generated record illustrates the mechanism; it is not an empirical accuracy study. Details.
The steady-state local-level Kalman gain here is
With , the limiting posterior variance has the same numerical value. By contrast, the static-state model with gives and . That decreasing gain is appropriate for a state that truly remains constant. Applied to the changing random walk, it builds confidence in the wrong model. The choice of process noise is therefore a statement about state evolution, rather than just an instruction to make a plot look smoother.

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