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### A Pluto.jl notebook ### | ||
# v0.20.17 | ||
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using Markdown | ||
using InteractiveUtils | ||
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# ╔═╡ a509f9d8-9c6d-11f0-3db9-cb5fe2e85d64 | ||
md"""# Constrained Optimization (Equality & Inequality KKT) | ||
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[⬅ Back to Class 02 Overview](class02_overview.jl) | ||
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[⬅ Previous: Unconstrained Minimization](class02_unconstrained_min.jl) | ||
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[➡ Next: Methods (Penalty/ALM/IPM)](class02_methods_barrier_alm.jl) | ||
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**In this section you will:** | ||
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* Build the **geometry** of equality constraints and the **KKT** conditions. | ||
* See the **Newton-on-KKT** linear system (saddle point) and when it’s well-posed. | ||
* Contrast **full Newton** vs. **Gauss–Newton** on the KKT system. | ||
* Extend to **inequality constraints** and understand **complementarity**. | ||
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""" | ||
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# ╔═╡ 57cd6d88-ea7e-4f5c-bc17-7fc65fb78e95 | ||
md"""## Equality-constrained minimization: geometry and conditions | ||
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**Problem:** | ||
[ | ||
\min_{x\in\mathbb{R}^n} f(x) \quad \text{s.t.}\quad C(x)=0,\ \ C:\mathbb{R}^n\to\mathbb{R}^m. | ||
] | ||
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**Geometric picture.** At an optimum on the manifold (C(x)=0), the negative gradient must lie in the tangent space: | ||
[ | ||
\nabla f(x^\star)\ \perp\ \mathcal{T}_{x^\star}={p:\ J_C(x^\star)p=0}. | ||
] | ||
Equivalently, the gradient is a linear combination of the constraint normals: | ||
[ | ||
\nabla f(x^\star)+J_C(x^\star)^{!T}\lambda^\star=0,\qquad C(x^\star)=0\quad(\lambda^\star\in\mathbb{R}^m). | ||
] | ||
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**Lagrangian.** (L(x,\lambda)=f(x)+\lambda^{!T}C(x)). | ||
""" | ||
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# ╔═╡ b7763163-fc68-4c56-bac9-c37de527858f | ||
md""" | ||
## Equality constraints: picture first | ||
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**Goal.** Minimize (f(x)) while staying on the surface (C(x)=0). | ||
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* **Feasible set as a surface.** Think of (C(x)=0) as a smooth surface embedded in (\mathbb{R}^n) (a manifold). | ||
* **Move without breaking the constraint.** Tangent directions are the “along-the-surface” moves keeping (C(x)) unchanged to first order. | ||
* **What must be true at the best point.** At (x^\star), there’s no downhill direction within the tangent space. | ||
* **Normals enter the story.** If the gradient can’t point along the surface, it must be balanced by the normals ({J_C(x^\star)_{i:}^{!T}}), producing multipliers (\lambda^\star). | ||
""" | ||
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# ╔═╡ 8a08b045-3a1b-4601-a081-27a6a22d05e6 | ||
md""" | ||
## From the picture to KKT (equality only) | ||
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For a regular local minimum: | ||
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1. **Feasibility:** (C(x^\star)=0). | ||
2. **Stationarity:** (\nabla f(x^\star) + J_C(x^\star)^{!T}\lambda^\star = 0). | ||
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**Lagrangian viewpoint.** Define (L(x,\lambda)=f(x)+\lambda^{!T}C(x)). At a solution, (x^\star) is stationary for (L) w.r.t. (x), while (C(x^\star)=0) ensures feasibility. | ||
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**Interpreting (\lambda^\star).** Each (\lambda_i^\star) reflects how strongly the (i)-th constraint “pushes back”; it’s also a sensitivity of the optimal value to perturbations in (C_i). | ||
""" | ||
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# ╔═╡ 907459d1-4a09-441c-a989-71ff687da873 | ||
md""" | ||
## KKT system for equalities (first order) & Newton on KKT | ||
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**KKT (FOC):** | ||
[ | ||
\nabla_x L(x,\lambda)=\nabla f(x)+J_C(x)^{!T}\lambda=0,\qquad C(x)=0. | ||
] | ||
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**Newton on KKT (linearize both blocks):** | ||
[ | ||
\begin{bmatrix} | ||
\nabla^2 f(x) + \sum_{i=1}^{m}\lambda_i,\nabla^2 C_i(x) & ; J_C(x)^{!T}[2pt] | ||
J_C(x) & ; 0 | ||
\end{bmatrix} | ||
\begin{bmatrix}\Delta x\ \Delta\lambda\end{bmatrix} | ||
=- | ||
\begin{bmatrix} | ||
\nabla f(x)+J_C(x)^{!T}\lambda[2pt] C(x) | ||
\end{bmatrix}. | ||
] | ||
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**Notes.** This is a symmetric **saddle-point** system. Practical solves use block elimination (Schur complement) and sparse factorizations. | ||
""" | ||
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# ╔═╡ aec59d16-c254-43b6-aee2-6261823fb7c3 | ||
md""" | ||
## Newton on KKT: practice & safeguards | ||
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**Works best when:** | ||
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* (J_C(x^\star)) has **full row rank** (regularity). | ||
* The **reduced Hessian** is **positive definite**. | ||
* A **globalization** (e.g., merit/penalty line search) and mild **regularization** are present. | ||
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**Common safeguards:** | ||
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* **Regularize** the ((1,1)) block (e.g., (+\beta I)) to ensure a good search direction. | ||
* **Merit/penalty line search** balancing feasibility vs. optimality. | ||
* **Scaling** constraints to improve conditioning of the KKT system. | ||
""" | ||
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# ╔═╡ a14a100c-5c92-42cc-899d-8c6eb0619368 | ||
md""" | ||
## Gauss–Newton vs. full Newton (equality case) | ||
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* **Full Newton Lagrangian Hessian:** | ||
[ | ||
\nabla_{xx}^2 L(x,\lambda)=\nabla^2 f(x)+\sum_{i=1}^m \lambda_i,\nabla^2 C_i(x). | ||
] | ||
* **Gauss–Newton approximation:** drop the constraint-curvature term: | ||
[ | ||
H_{\text{GN}}(x)\approx \nabla^2 f(x). | ||
] | ||
Comment on lines
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There was a problem hiding this comment. Choose a reason for hiding this commentThe reason will be displayed to describe this comment to others. Learn more. I'm not sure this is correct. GN is for nonlinear least squares, not constrained opt? I could be wrong. please clarify |
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**Trade-offs.** | ||
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* **Full Newton:** fewer iterations near the solution; costlier steps; less robust far away. | ||
* **Gauss–Newton:** cheaper per step and often more stable; may need more iterations but competitive in wall-clock on many problems. | ||
""" | ||
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# ╔═╡ 300c917e-e61c-4881-82d0-bc79ace66795 | ||
md""" | ||
## Solving the KKT system: Schur complement (intuition) | ||
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Given | ||
[ | ||
\begin{bmatrix} H & A^{!T}\ A & 0\end{bmatrix} | ||
\begin{bmatrix}\Delta x\ \Delta\lambda\end{bmatrix} | ||
=- | ||
\begin{bmatrix} g\ c\end{bmatrix}, | ||
] | ||
with (H\approx \nabla_{xx}^2 L), (A=J_C(x)), (g=\nabla f+J_C^{!T}\lambda), (c=C(x)). | ||
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* Eliminate (\Delta x): (\Delta x = -H^{-1}(g + A^{!T}\Delta\lambda)). | ||
* Schur system in (\Delta\lambda): | ||
[ | ||
(A H^{-1} A^{!T}),\Delta\lambda = c + A H^{-1} g. | ||
] | ||
* Then recover (\Delta x). | ||
Exploit **sparsity**: factor (H) once per iteration; reuse structure across iterations. | ||
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""" | ||
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# ╔═╡ 28a43bca-618a-4fec-a7eb-ad7a734ceac5 | ||
md""" | ||
## Inequality-constrained minimization and KKT | ||
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**Problem:** (\min f(x)\ \text{s.t.}\ c(x)\ge 0,\ \ c:\mathbb{R}^n\to\mathbb{R}^p). | ||
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**KKT (FOC):** | ||
[ | ||
\begin{aligned} | ||
&\text{Stationarity:} && \nabla f(x)-J_c(x)^{!T}\lambda=0,\ | ||
&\text{Primal feasibility:} && c(x)\ge 0,\ | ||
&\text{Dual feasibility:} && \lambda\ge 0,\ | ||
&\text{Complementarity:} && \lambda^{!T}c(x)=0\quad(\lambda_i c_i(x)=0,\ \forall i). | ||
\end{aligned} | ||
] | ||
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**Interpretation.** | ||
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* **Active** constraints: (c_i(x)=0\Rightarrow \lambda_i) can be nonzero (acts like an equality). | ||
* **Inactive** constraints: (c_i(x)>0\Rightarrow \lambda_i=0) (no influence on stationarity). | ||
""" | ||
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# ╔═╡ 3b6300c0-d69f-4004-9b91-41116d0ce832 | ||
md""" | ||
## Complementarity: intuition & Newton’s challenge | ||
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**What (\lambda_i c_i(x)=0) means.** | ||
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* Tight constraint ((c_i=0)) → can press back ((\lambda_i\ge 0)). | ||
* Loose constraint ((c_i>0)) → no force ((\lambda_i=0)). | ||
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**Why naïve Newton struggles.** | ||
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* Complementarity brings **nonsmoothness** and **inequalities** ((\lambda\ge 0), (c(x)\ge 0)). | ||
* Equality-style Newton can violate nonnegativity or bounce across the boundary. | ||
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**Two main strategies (preview).** | ||
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* **Active-set:** guess actives → solve equality-constrained subproblem → update the set. | ||
* **Barrier / PDIP / ALM:** smooth or relax complementarity, use damped Newton, and drive the relaxation to zero. | ||
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""" | ||
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# ╔═╡ ab782dbb-5f3c-404f-87b7-091b4382b0aa | ||
md""" | ||
## Globalization with constraints: merit functions | ||
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To balance feasibility and optimality during updates ((x,\lambda)\to(x+\alpha\Delta x,\lambda+\alpha\Delta\lambda)), use a **merit/penalty** function, e.g. | ||
[ | ||
\Phi_\mu(x) = f(x) + \mu,|C(x)|*1 \quad \text{(equality case)}, | ||
] | ||
or for inequalities, a penalty on **violation** (v(x)=\sum_i \max(0,-c_i(x))). | ||
Do a **backtracking line search** on (\Phi*\mu) to ensure robust progress. | ||
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*(You’ll see barrier and ALM variants in the next section.)* | ||
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""" | ||
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# ╔═╡ 0f722888-d66c-47ae-a1ee-1e2b7c9b4a58 | ||
md""" | ||
## Conditioning & scaling | ||
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* **Scale constraints** so rows of (J_C) have comparable norms → better KKT conditioning. | ||
* **Regularize** (H) when indefinite/ill-conditioned (modified Cholesky or (+\beta I)). | ||
* **Exploit structure:** block-banded, sparse patterns common in trajectory problems. | ||
* **Warm-starts** from previous solves (e.g., along continuation or time steps) improve robustness. | ||
""" | ||
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# ╔═╡ f4d85409-9095-4bc0-b515-ae283e43f344 | ||
md""" | ||
## Where to next | ||
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* Proceed to **Methods: Penalty vs. Augmented Lagrangian vs. Interior-Point** to see practical algorithms that *enforce* the KKT conditions reliably, including complementarity handling for inequalities. | ||
* Later, we’ll assemble these pieces into **SQP**. | ||
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[➡ Methods (Penalty/ALM/IPM) (next)](class02_methods_barrier_alm.jl) · [⬅ Back to overview](class02_overview.jl) | ||
""" | ||
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# ╔═╡ 00000000-0000-0000-0000-000000000001 | ||
PLUTO_PROJECT_TOML_CONTENTS = """ | ||
[deps] | ||
""" | ||
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# ╔═╡ 00000000-0000-0000-0000-000000000002 | ||
PLUTO_MANIFEST_TOML_CONTENTS = """ | ||
# This file is machine-generated - editing it directly is not advised | ||
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julia_version = "1.10.0" | ||
manifest_format = "2.0" | ||
project_hash = "da39a3ee5e6b4b0d3255bfef95601890afd80709" | ||
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[deps] | ||
""" | ||
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# ╔═╡ Cell order: | ||
# ╠═a509f9d8-9c6d-11f0-3db9-cb5fe2e85d64 | ||
# ╠═57cd6d88-ea7e-4f5c-bc17-7fc65fb78e95 | ||
# ╠═b7763163-fc68-4c56-bac9-c37de527858f | ||
# ╠═8a08b045-3a1b-4601-a081-27a6a22d05e6 | ||
# ╠═907459d1-4a09-441c-a989-71ff687da873 | ||
# ╠═aec59d16-c254-43b6-aee2-6261823fb7c3 | ||
# ╠═a14a100c-5c92-42cc-899d-8c6eb0619368 | ||
# ╠═300c917e-e61c-4881-82d0-bc79ace66795 | ||
# ╠═28a43bca-618a-4fec-a7eb-ad7a734ceac5 | ||
# ╠═3b6300c0-d69f-4004-9b91-41116d0ce832 | ||
# ╠═ab782dbb-5f3c-404f-87b7-091b4382b0aa | ||
# ╠═0f722888-d66c-47ae-a1ee-1e2b7c9b4a58 | ||
# ╠═f4d85409-9095-4bc0-b515-ae283e43f344 | ||
# ╟─00000000-0000-0000-0000-000000000001 | ||
# ╟─00000000-0000-0000-0000-000000000002 |
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Consider adding a figure for this