Inferensys

Glossary

Excitation Trajectory

An excitation trajectory is a deliberately designed sequence of control inputs or motions for a robotic system that persistently excites all relevant dynamic modes to enable accurate system identification.
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SYSTEM IDENTIFICATION

What is an Excitation Trajectory?

A core concept in robotics and control theory for building accurate dynamic models from data.

An excitation trajectory is a deliberately designed sequence of control inputs or motions for a robotic system that is rich enough to persistently excite all relevant dynamic modes, enabling accurate system identification. It is engineered to generate data that reveals the system's underlying physics, such as inertia, friction, and Coriolis forces, by ensuring the input signal's frequency content and amplitude span the operational range. Without sufficient excitation, key parameters remain unobservable, leading to poor model fidelity and a wider reality gap.

The design of an effective excitation trajectory balances controllability and observability while respecting physical constraints like joint limits and torque saturation. Common techniques include using sum-of-sinusoids, chirp signals, or optimized pseudo-random sequences. The resulting data is used in a system ID pipeline with a dynamic regressor to perform parameter estimation, directly feeding into simulation calibration and reducing model uncertainty. This process is foundational for sim-to-real transfer, as a well-identified model minimizes simulation bias and transfer error.

SYSTEM IDENTIFICATION

Key Characteristics of an Effective Excitation Trajectory

For accurate system identification, an excitation trajectory must be deliberately designed to reveal the full dynamic behavior of the robotic system. The following characteristics define an optimal trajectory for parameter estimation.

01

Persistent Excitation

Persistent excitation is the fundamental property that an input signal must possess to enable the consistent identification of all system parameters. A trajectory is persistently exciting if it provides sufficient stimulation across all dynamic modes and frequencies of interest over the entire data collection period. This ensures the regression matrix in the identification algorithm remains well-conditioned, preventing numerical ill-posedness and guaranteeing that all unknown parameters (e.g., inertia, friction coefficients) are uniquely identifiable from the collected data.

02

Sufficient Spectral Content

The trajectory must contain a broad frequency spectrum to excite the system's natural dynamics. This is often achieved by designing signals that are sums of sinusoids or via chirp signals that sweep through a target frequency band.

  • Low-frequency content is needed to identify parameters related to gravity and static friction.
  • Mid-to-high-frequency content is required to identify inertial and Coriolis effects.
  • The bandwidth of the excitation must exceed the closed-loop bandwidth expected during normal operation to ensure the identified model is valid for subsequent controller design.
03

Adequate Amplitude and Duration

The signal must have sufficient amplitude to produce measurable outputs above the noise floor of the sensors, ensuring a high signal-to-noise ratio. However, amplitudes must remain within the safe operational limits of the hardware to avoid damage. The duration must be long enough to capture transient responses and allow for the decay of initial condition effects, providing multiple cycles of the lowest frequency components. For a robotic arm, this often means the trajectory should move all joints through a significant portion of their workspace.

04

Optimal Experiment Design

This involves designing the trajectory to maximize the Fisher information matrix or minimize the covariance of the parameter estimates. The goal is to make the estimation problem as well-conditioned as possible. Common optimality criteria include:

  • D-optimality: Maximizes the determinant of the information matrix, minimizing the volume of the confidence ellipsoid for the parameters.
  • A-optimality: Minimizes the trace of the parameter covariance matrix.
  • E-optimality: Maximizes the minimum eigenvalue of the information matrix. These criteria often result in trajectories that appear random or pseudo-random but are mathematically optimized for precision.
05

Physical Feasibility and Safety

The designed trajectory must respect all actuator limits (torque, velocity, acceleration) and joint limits of the physical robot. It must avoid configurations that lead to singularities or self-collision. For safety, the trajectory is often executed under high-gain position control or in a gravity-compensation mode before moving to torque control for data collection. This characteristic ensures the experiment is repeatable and does not damage the hardware, which is critical for industrial and research applications.

06

Common Trajectory Types

Several standard trajectory classes are used in practice:

  • Sum-of-Sinusoids: A linear combination of sine waves at different frequencies, allowing precise control over spectral content.
  • Pseudo-Random Binary Sequence (PRBS): A signal that switches between two levels in a random but repeatable pattern, providing wideband excitation.
  • Chirp Signal: A sine wave with a frequency that increases or decreases linearly over time, efficiently sweeping a frequency band.
  • Optimal Robotic Excitations: Trajectories parameterized by Fourier series or polynomial coefficients, where the coefficients are optimized directly for a system identification criterion (e.g., D-optimality).
SYSTEM IDENTIFICATION

How is an Excitation Trajectory Designed?

An excitation trajectory is a deliberately designed sequence of control inputs or motions for a robotic system that is rich enough to persistently excite all relevant dynamic modes, enabling accurate system identification.

Design begins with defining the dynamic regressor, a linear matrix formulation derived from the system's equations of motion. The trajectory must ensure persistent excitation across all unknown parameters like inertia and friction. This is achieved by optimizing the input sequence—often via Fourier series or optimized point-to-point motions—to maximize the information content in the collected data while respecting the robot's physical actuator limits and safety constraints.

The optimized trajectory is executed on the physical hardware, and the resulting input-output data is recorded. This data is then used in the parameter estimation step of the system identification pipeline. A well-designed trajectory minimizes the covariance of the parameter estimates, leading to a highly accurate dynamic model that is essential for high-performance model-based control and for reducing the reality gap in sim-to-real transfer.

EXPERIMENT DESIGN

Common Excitation Trajectory Techniques

Excitation trajectories are deliberately designed control sequences that persistently stimulate a system's dynamic modes to enable accurate parameter estimation. The choice of technique balances identification accuracy, experimental safety, and computational efficiency.

01

Swept-Sine (Chirp) Signals

A swept-sine or chirp signal is a sinusoidal input whose frequency increases (or decreases) linearly or logarithmically over time. This technique is foundational for frequency-domain system identification.

  • Primary Use: Excites a broad, continuous band of frequencies to characterize the system's frequency response and resonant modes.
  • Key Property: Provides excellent persistent excitation across the specified bandwidth, ensuring all relevant dynamic modes are stimulated.
  • Implementation: Defined as (u(t) = A \sin(2\pi (f_0 + kt) t)), where (f_0) is the start frequency and (k) is the sweep rate. Logarithmic sweeps are often used to ensure equal energy per octave.
  • Advantage: Directly reveals system bandwidth and phase margins. It is a standard signal for identifying transfer functions in linear time-invariant systems.
02

Pseudo-Random Binary Sequence (PRBS)

A Pseudo-Random Binary Sequence is a deterministic, noise-like signal that switches between two predefined amplitude levels according to a maximum-length shift register sequence.

  • Primary Use: Excites a wide spectrum of frequencies with a signal that has well-defined statistical properties and is safe for amplitude-limited actuators.
  • Key Property: Its autocorrelation function approximates a Dirac delta function, making it spectrally similar to white noise but with bounded amplitude.
  • Implementation: The sequence length (L = 2^n - 1) (where (n) is the register order) determines the frequency resolution. The clock period sets the highest excited frequency.
  • Advantage: Maximizes signal power within actuator saturation limits, providing high signal-to-noise ratio for parameter estimation while maintaining safe operating conditions.
03

Multi-Sine (Sum of Sines) Signals

A multi-sine signal is a sum of sinusoids at specific, non-harmonically related frequencies, with carefully chosen phases and amplitudes.

  • Primary Use: Provides precise control over which frequencies are excited, allowing targeted probing of the system's dynamics at points of interest.
  • Key Property: Enforces persistent excitation at a discrete set of frequencies. Phase optimization (e.g., using Schroeder phases) minimizes the crest factor (peak-to-RMS ratio), distributing energy efficiently.
  • Implementation: (u(t) = \sum_{k=1}^{N} A_k \sin(2\pi f_k t + \phi_k)). The frequencies (f_k) are chosen based on prior knowledge of the system's bandwidth.
  • Advantage: Enables non-parametric frequency response estimation at the chosen points with high accuracy and allows for the separation of linear and nonlinear dynamics in the response.
04

Optimal Experiment Design

Optimal experiment design formulates the trajectory generation as an optimization problem to maximize the information content in the collected data for parameter estimation.

  • Primary Use: To design trajectories that minimize the statistical uncertainty (covariance) of the estimated parameters, subject to physical constraints.
  • Key Objective: Maximize a criterion based on the Fisher Information Matrix (FIM), such as D-optimality (maximizing the determinant of the FIM) or E-optimality (maximizing its minimum eigenvalue).
  • Constraints: The optimization incorporates actuator torque/velocity limits, joint position limits, and collision avoidance to ensure the trajectory is executable and safe.
  • Advantage: Produces the most informative data possible within the system's operational envelope, leading to the highest possible parameter estimation accuracy for a given experiment duration.
05

Dynamic Regressor-Based Trajectories

This technique designs trajectories that ensure the dynamic regressor matrix—which linearly maps parameters to torque—is well-conditioned for the specific parameters of interest.

  • Primary Use: Directly targets the identifiability of inertial and friction parameters in rigid-body dynamics models, such as the Newton-Euler or Lagrangian formulations.
  • Core Principle: The robot's equations of motion can be written linearly in the dynamic parameters: (\tau = Y(q, \dot{q}, \ddot{q}) \pi), where (Y) is the regressor and (\pi) is the parameter vector. The trajectory is designed to make (Y) full rank.
  • Method: Often involves solving an optimization to maximize the minimum singular value of the aggregated regressor matrix over the trajectory, ensuring all columns of (Y) are independently excited.
  • Advantage: Provides guarantees on parameter estimation convergence for the specific dynamic model and is the standard method for high-precision inertial parameter identification in robotics.
06

Task-Space Excitation

Task-space excitation designs motions in the robot's operational space (e.g., Cartesian end-effector paths) that indirectly create rich joint-space excitation.

  • Primary Use: To identify parameters relevant to task performance (like tool dynamics) or when joint-space trajectories are constrained by the workspace.
  • Method: Defines excitation paths like figure-eights, Lissajous curves, or random walks in Cartesian space. The inverse kinematics solution generates the corresponding joint trajectory.
  • Consideration: Must account for kinematic singularities and the non-linear mapping from task to joint space, which can affect the persistence of excitation.
  • Advantage: Directly excites the dynamics in the coordinate frame where the robot is controlled and performs its primary function, aligning the identification experiment with the ultimate use case.
EXCITATION TRAJECTORY

Frequently Asked Questions

An excitation trajectory is a deliberately designed sequence of control inputs or motions for a robotic system that is rich enough to persistently excite all relevant dynamic modes, enabling accurate system identification. This FAQ addresses common questions about its design, purpose, and role in simulation fidelity.

An excitation trajectory is a deliberately designed sequence of control inputs or motions for a robotic system that is rich enough to persistently excite all relevant dynamic modes, enabling accurate system identification. It works by commanding the robot through a varied set of movements—often involving rapid accelerations, decelerations, and motions through the full range of its workspace—to generate informative data. This data, when fed into parameter estimation algorithms, allows engineers to solve for unknown physics parameters like link masses, inertias, and friction coefficients. The trajectory must be sufficiently complex to make the system's dynamics observable in the collected sensor data, ensuring the identification problem is well-posed and yields a unique, accurate solution.

Prasad Kumkar

About the author

Prasad Kumkar

CEO & MD, Inference Systems

Prasad Kumkar is the CEO & MD of Inference Systems and writes about AI systems architecture, LLM infrastructure, model serving, evaluation, and production deployment. Over 5+ years, he has worked across computer vision models, L5 autonomous vehicle systems, and LLM research, with a focus on taking complex AI ideas into real-world engineering systems.

His work and writing cover AI systems, large language models, AI agents, multimodal systems, autonomous systems, inference optimization, RAG, evaluation, and production AI engineering.