Consider the following autonomous nonlinear system:

where
denotes the system state vector. Also,
and
's are known analytic vector functions, and
is the
element of an unknown disturbance to the system.
At the desired nominal point, the nonlinear functions in the above system can be approximated by Taylor expansion
![{\displaystyle f(x)\simeq f(x_{0})+\sum _{k=1}^{\eta }{\frac {1}{k!}}\partial f_{[k]}\mid _{x=x_{0}}(x-x_{0})^{[k]}}](//wikimedia.org/api/rest_v1/media/math/render/svg/e84b18169cca116cea6b7cab49bd085358d2edf6)
where
is the
partial derivative of
with respect to
at
and
denotes the
Kronecker product.
Without loss of generality, we assume that
is at the origin.
Applying Taylor approximation to the system, we obtain
![{\displaystyle {\dot {x}}\simeq \sum _{k=0}^{\eta }A_{k}x^{[k]}+\sum _{j=1}^{m}\sum _{k=0}^{\eta }B_{jk}x^{[k]}d_{j}}](//wikimedia.org/api/rest_v1/media/math/render/svg/d5eb8aa70fda330af34e5bcbda4f70e8aa875779)
where
and
.
Consequently, the following linear system for higher orders of the original states are obtained:
![{\displaystyle {\frac {d(x^{[i]})}{dt}}\simeq \sum _{k=0}^{\eta -i+1}A_{i,k}x^{[k+i-1]}+\sum _{j=1}^{m}\sum _{k=0}^{\eta -i+1}B_{j,i,k}x^{[k+i-1]}d_{j}}](//wikimedia.org/api/rest_v1/media/math/render/svg/dd0b8b3adffc2c4d6bacf9eb517a4471755af0a3)
where
, and similarly
.
Employing Kronecker product operator, the approximated system is presented in the following form
![{\displaystyle {\dot {x}}_{\otimes }\simeq Ax_{\otimes }+\sum _{j=1}^{m}[B_{j}x_{\otimes }d_{j}+B_{j0}d_{j}]+A_{r}}](//wikimedia.org/api/rest_v1/media/math/render/svg/65d5ed5157c6aaaa06fa46899e1a2f24fccf5fa6)
where
, and
and
matrices are defined in (Hashemian and Armaou 2015).[6]