SyncValsverifier → artifact → classifier → verdict
SyncVals · Trajectory

beam-deflection-solver

claude-code claude-opus-4-8 ✗ failed GOOD_FAILURE ↑ View task
Solved from the instruction alone, tests/ and solution/ were withheld from the agent's workspace and restored only for grading.
Reward = tests/test.sh exit code (0 → resolved); the classification below is post-hoc and cannot change it.
Classification , post-hoc; cannot change the reward
GOOD_FAILUREHonest miss, the agent ran correctly but couldn't solve it. Expected for a hard task; the task is sound.
SubtypeImplementation Bugs
EvidenceThe hidden test suite shows: "[ FAIL ] invariant_symmetry: symmetry at node 0". The agent's implementation assembles a finite-difference system and passes 3/4 invariant tests (equilibrium_residual, mechanism_rejection, input_validation), but fails the symmetry invariant. The agent's local testing only ran a subset of tests (1 test passed) while the hidden suite runs 4 tests. The agent claimed correct implementation but did not validate against the full hidden test suite that checks fundamental invariants like symmetry preservation, which are implicit requirements for a correct finite-difference scheme even if not explicitly stated in instruction.md.
Root causeThe agent implemented a finite-difference scheme that passes local smoke tests and three of four invariant checks, but the boundary condition or discretization treatment breaks symmetry preservation at node 0. This indicates an implementation error in how boundary conditions are applied or how the stencil handles symmetric loadings, not a task specification issue.
RecommendationN/A - task is fine. The task is properly specified with clear physics, discretization requirements (second-order accuracy), and boundary condition semantics. The oracle passes all tests including symmetry. The agent's failure is due to an implementation bug in boundary condition handling or stencil formulation that breaks symmetry preservation, a fundamental property that any correct finite-difference solver should maintain for symmetric problems, even if not explicitly mentioned in the instruction.
Trajectory
Tool-by-tool agent trajectory
27 tool calls · 4 tool types · 43 steps
# Ticket: Implement the finite-difference core for the BeamFD bending solver ## Context `beamfd` is a small C++17 structural-analysis engine that computes the static transverse deflection of an **Euler-Bernoulli beam** that may have a **non-uniform flexural rigidity `EI(x)`**, may rest on an elastic (Winkler) **foundation `k(x)`**, and may carry a spatially varying distributed load `q(x)` together with forces or moments applied at free ends. The surrounding framework is complete and must be reused: - `Beam` , geometry, the per-node fields, and support/load data, with accessors `EI_at(i)`, `k_at(i)`, `q_at(i)`, `end_moment(left)`, `applied_end_shear(left)`, `left()`, `right()`, `dx()`, `num_intervals()`, `num_nodes()`, `node_x(i)`, and `validate()`. - `DenseMatrix` and `solve_general(A, b)` , a dense linear-algebra layer with a general (non-symmetric) LU solver. - `io` , the `.beam` text parser and report writer; a demo CLI. - The deflection-recovery helpers on the solver (`bending_moment_field`, `shear_field`) are already implemented. The numerical core , the **finite-difference discretization** , is unimplemented. Its two member functions are stubs that return a zero/empty system, so the engine reports a beam that does not deflect. The project is at **`/opt/beamfd`** in the build image. ## Your task Implement the two stubbed member functions in **`/opt/beamfd/src/solver.cpp`** (declared in `include/beamfd/solver.hpp`): - `BeamSystem BeamSolver::assemble_system() const` - `BeamResult BeamSolver::solve() const` **Do not change the public headers / signatures**, do **not** modify the already-implemented recovery helpers, and reuse the existing support layer. You should only need to edit `src/solver.cpp`. ## Governing physics (small-deflection, static) The transverse deflection `w(x)` on `x in [0, L]` satisfies the conservative (divergence) form of the Euler-Bernoulli bending equation with an elastic foundation: ``` d²/dx² ( EI(x) · d²w/dx² ) + k(x) · w(x) = q(x) ``` - `EI(x) > 0` is the flexural rigidity field `[N·m²]` (generally **not** constant). - `k(x) >= 0` is the Winkler foundation modulus `[N/m²]` (0 where there is no foundation). - `q(x)` is the distributed transverse load `[N/m]`. - `w` is the deflection `[m]`. The bending moment is `M = EI(x) w''` `[N·m]` and the shear is `V = (EI(x) w'')'` `[N]`. Note that when `EI` varies in space the fourth-order operator is **not** simply `EI · w''''`; it is the second derivative of `EI(x) w''(x)`. ## Boundary and support semantics Each end carries two conditions, set by its support type: - **Clamped**: `w = 0` and `w' = 0` (prescribed deflection and slope). - **Pinned**: `w = 0` and `M = EI w'' = 0` (prescribed deflection, zero moment). - **Free**: `M = EI w'' = M_applied` and `V = (EI w'')' = V_applied`, where the applied moment/shear come from `Beam::end_moment(...)` and `Beam::applied_end_shear(...)` (both zero when nothing is applied). Determinacy: a free end must be balanced by enough restraint. With no foundation, a free end requires a clamped opposite end; a free-free or free-pinned beam is a rigid-body **mechanism**. A non-trivial foundation `k(x)` supplies distributed restraint that makes any support combination well posed. `Beam::validate()` encodes these rules and throws for an unsupported (mechanism) configuration. ## Discretization requirement (you choose the scheme) Work on the uniform grid `x_i = i·dx`, `i = 0..N`, `dx = L/N`, with `n = N+1` nodal unknowns `w_i = w(x_i)`. Assemble the linear system `A w = b` for the nodal deflections that discretizes the governing equation and its boundary conditions, and solve it with `solve_general`. Use a scheme that is at least **second-order accurate** in `dx`; the boundary conditions (essential ones at clamped/pinned ends, natural ones at free ends) must be incorporated consistently with the same order. Deriving an appropriate stencil and boundary treatment is the substance of the task. ## Contract / edge cases - `solve()` must call `Beam::validate()` first and let its exceptions propagate. - If the assembled system is singular, let the exception from `solve_general` propagate out of `solve()`. - `assemble_system()` returns `A` of size `num_nodes × num_nodes` and `b` of length `num_nodes`. - `deflection` has length `num_nodes()`, ordered from `x = 0` (i = 0) to `x = L` (i = N). ## `.beam` input format (handled by `io`; for reference) ``` length <L> # span [m] cells <n> # number of equal intervals (>= 2) support <left> <right> # each of: clamped | pinned | free ei <EI> # constant flexural rigidity, OR: ei_profile <x0> <v0> <x1> <v1> ... # piecewise-linear EI(x) foundation <k> # constant Winkler modulus [N/m^2] (optional) foundation_profile <x0> <v0> ... # piecewise-linear k(x) (optional) udl <q> # uniform load [N/m] (optional) load <x0> <x1> <q0> <q1> # piecewise-linear load segment (repeatable) endload <left|right> <P> # transverse force at a free end [N] (optional) endmoment <left|right> <M> # moment at a free end [N*m] (optional) ``` ## Build & test ``` cmake -S /opt/beamfd -B /opt/beamfd/build -DCMAKE_BUILD_TYPE=Release cmake --build /opt/beamfd/build --parallel cd /opt/beamfd/build && ctest --output-on-failure ``` The shipped test is only a small **smoke** check; the authoritative grading is a separate **hidden** suite that verifies accuracy against independently manufactured solutions and second-order mesh convergence across the supported support types, variable-EI profiles, foundations and end actions. Tolerances are intentionally not published , aim for a correct, convergent discretization rather than fitting any specific number.
I'll start by exploring the project structure to understand the framework I need to work with.

/opt/beamfd/src/solver.cpp

contents
1	#include "beamfd/solver.hpp"
2	
3	#include <cmath>
4	#include <cstddef>
5	#include <stdexcept>
6	#include <vector>
7	
8	#include "beamfd/linalg.hpp"
9	#include "beamfd/types.hpp"
10	
11	namespace beamfd {
12	
13	// ============================================================================
14	// TODO(candidate): Implement the beam-bending finite-difference core.
15	//
16	// Two member functions below are stubs that currently return a zero deflection
17	// field and an empty/zero system, so every analysis is wrong and the grader
18	// fails. Replace the stub bodies of
19	//
20	//     BeamSystem BeamSolver::assemble_system() const;
21	//     BeamResult BeamSolver::solve()          const;
22	//
23	// with correct implementations of the boundary-value problem specified in
24	// instruction.md. Do NOT change the public signatures declared in
25	// include/beamfd/solver.hpp, do NOT modify the recovery helpers below, and
26	// reuse the existing support layer (DenseMatrix, solve_general, and the Beam
27	// accessors EI_at / k_at / q_at / end_moment / applied_end_shear / left /
28	// right / dx / num_intervals / num_nodes / validate).
29	//
30	// The physics, the support and load semantics, the contract, and the I/O
31	// format are described in instruction.md. The required behaviour is enforced
32	// by a hidden grading suite (the shipped tests/ are only a smoke check); design
33	// a discretization that is at least second-order accurate and assemble the
34	// linear system A w = b for the nodal deflection, then solve it with
35	// solve_general. Call Beam::validate() at the start of solve() and let its
36	// exceptions (and any singular-system exception from solve_general) propagate.
37	// ============================================================================
38	
39	BeamSystem BeamSolver::assemble_system() const {
40	    // TODO(candidate): build and return the finite-difference system A w = b.
41	    const std::size_t n = beam_.num_nodes();
42	    BeamSystem sys;
43	    sys.A = DenseMatrix(n, n);  // all zeros -> singular / wrong
44	    sys.b.assign(n, 0.0);
45	    return sys;
46	}
47	
48	BeamResult BeamSolver::solve() const {
49	    // TODO(candidate): validate, assemble, solve, return the deflection field.
50	    const std::size_t n = beam_.num_nodes();
51	    BeamResult result;
52	    result.deflection.assign(n, 0.0);  // trivially zero -> wrong
53	    return result;
54	}
55	
56	// ----------------------------------------------------------------------------
57	// Recovery helpers (already implemented; do NOT modify). These differentiate a
58	// given deflection field so callers can recompute physical quantities (bending
59	// moment, shear) directly from a candidate result, honoring a variable EI(x).
60	
61	namespace {
62	
63	// Second derivative w''(x_i) by central difference (interior) / one-sided
64	// 2nd-order difference (ends).
65	double second_derivative(const std::vector<double>& w, std::size_t i, double h2) {
66	    const std::size_t n = w.size();
67	    if (i == 0) {
68	        return (2.0 * w[0] - 5.0 * w[1] + 4.0 * w[2] - w[3]) / h2;
69	    }
70	    if (i == n - 1) {
71	        return (2.0 * w[n - 1] - 5.0 * w[n - 2] + 4.0 * w[n - 3] - w[n - 4]) / h2;
72	    }
73	    return (w[i - 1] - 2.0 * w[i] + w[i + 1]) / h2;
74	}
75	
76	} // namespace
77	
78	std::vector<double> BeamSolver::bending_moment_field(
79	    const std::vector<double>& w) const {
80	    const std::size_t n = beam_.num_nodes();
81	    if (w.size() != n) {
82	        throw std::invalid_argument("bending_moment_field: deflection size mismatch");
83	    }
84	    const double h2 = beam_.dx() * beam_.dx();
85	    std::vector<double> M(n, 0.0);
86	    for (std::size_t i = 0; i < n; ++i) {
87	        M[i] = beam_.EI_at(i) * second_derivative(w, i, h2);
88	    }
89	    return M;
90	}
91	
92	std::vector<double> BeamSolver::shear_field(const std::vector<double>& w) const {
93	    const std::size_t n = beam_.num_nodes();
94	    if (w.size() != n) {
95	        throw std::invalid_argument("shear_field: deflection size mismatch");
96	    }
97	    if (n < 5) {
98	        throw std::invalid_argument("shear_field: need at least 5 nodes");
99	    }
100	    const double h = beam_.dx();
101	    const double h2 = h * h;
102	    std::vector<double> m(n, 0.0);
103	    for (std::size_t j = 0; j < n; ++j) {
104	        m[j] = beam_.EI_at(j) * second_derivative(w, j, h2);
105	    }
106	    std::vector<double> V(n, 0.0);
107	    for (std::size_t i = 0; i < n; ++i) {
108	        if (i == 0) {
109	            V[i] = (-3.0 * m[0] + 4.0 * m[1] - m[2]) / (2.0 * h);
110	        } else if (i == n - 1) {
111	            V[i] = (3.0 * m[n - 1] - 4.0 * m[n - 2] + m[n - 3]) / (2.0 * h);
112	        } else {
113	            V[i] = (m[i + 1] - m[i - 1]) / (2.0 * h);
114	        }
115	    }
116	    return V;
117	}
118	
119	} // namespace beamfd
120

/opt/beamfd/include/beamfd/solver.hpp

contents
1	#ifndef BEAMFD_SOLVER_HPP
2	#define BEAMFD_SOLVER_HPP
3	
4	#include <cstddef>
5	#include <vector>
6	
7	#include "beamfd/beam.hpp"
8	#include "beamfd/linalg.hpp"
9	
10	namespace beamfd {
11	
12	/// The assembled finite-difference linear system A w = b for a beam.
13	/// `A` has size num_nodes x num_nodes and `b` has length num_nodes; the
14	/// unknown w is the nodal transverse deflection field. Exposed so tests can
15	/// check the discrete equilibrium residual directly.
16	struct BeamSystem {
17	    DenseMatrix A;
18	    std::vector<double> b;
19	};
20	
21	/// Result of a static beam-bending analysis.
22	struct BeamResult {
23	    /// Nodal transverse deflection w_i [m], length == beam.num_nodes(),
24	    /// ordered from x = 0 (i = 0) to x = L (i = num_intervals).
25	    std::vector<double> deflection;
26	};
27	
28	/// Static bending solver for an Euler-Bernoulli beam with (possibly) variable
29	/// flexural rigidity and an optional elastic foundation. The continuum
30	/// boundary-value problem and the support/load semantics are specified in
31	/// instruction.md; choosing and assembling a suitable finite-difference
32	/// discretization of it, and solving the resulting linear system, is the work
33	/// of this class.
34	class BeamSolver {
35	public:
36	    explicit BeamSolver(const Beam& beam) : beam_(beam) {}
37	
38	    /// Run the full analysis. Calls Beam::validate() first and propagates any
39	    /// exception it throws. Throws std::runtime_error if the assembled system
40	    /// is singular.
41	    BeamResult solve() const;
42	
43	    /// Assemble the finite-difference system A w = b. Exposed for testing and
44	    /// reuse (the discrete equilibrium-residual invariant checks A w - b ~ 0 at
45	    /// the interior nodes).
46	    BeamSystem assemble_system() const;
47	
48	    // ---- Recovery helpers (fully implemented; operate on a deflection field).
49	    // These let the caller recompute physical quantities directly from a
50	    // candidate deflection vector, independent of how it was produced.
51	
52	    /// Bending moment M_i = EI(x_i) * w''(x_i) [N*m] via a central second
53	    /// difference at interior nodes and a one-sided second difference at the
54	    /// ends. `w` must have length num_nodes(). Throws std::invalid_argument
55	    /// otherwise.
56	    std::vector<double> bending_moment_field(const std::vector<double>& w) const;
57	
58	    /// Shear force V_i = (EI w'')'(x_i) [N] via finite differences of the
59	    /// nodal bending moment. `w` must have length num_nodes(). Throws
60	    /// std::invalid_argument otherwise.
61	    std::vector<double> shear_field(const std::vector<double>& w) const;
62	
63	private:
64	    const Beam& beam_;
65	};
66	
67	} // namespace beamfd
68	
69	#endif // BEAMFD_SOLVER_HPP
70
Now let me look at the Beam and linalg headers to understand the available accessors.

/opt/beamfd/include/beamfd/beam.hpp

contents
1	#ifndef BEAMFD_BEAM_HPP
2	#define BEAMFD_BEAM_HPP
3	
4	#include <cstddef>
5	#include <utility>
6	#include <vector>
7	
8	#include "beamfd/types.hpp"
9	
10	namespace beamfd {
11	
12	/// A 1D Euler-Bernoulli beam discretized on a uniform grid, with a possibly
13	/// non-uniform flexural rigidity EI(x), an optional Winkler elastic foundation
14	/// k(x), a (possibly spatially varying) transverse load q(x), and optional
15	/// applied force/moment at free ends.
16	///
17	/// This is a plain data container plus light validation. The numerical core
18	/// (assembling and solving the finite-difference system for the deflection
19	/// field) lives in BeamSolver (see solver.hpp).
20	///
21	/// Geometry / grid:
22	///   - The beam occupies x in [0, L], divided into `num_intervals` equal cells,
23	///     giving num_nodes() = num_intervals + 1 grid points at x_i = i * dx,
24	///     dx = L / num_intervals, for i = 0 .. num_intervals.
25	///
26	/// Fields are stored per node (length num_nodes()):
27	///   - EI_at(i)  flexural rigidity at node i  [N*m^2]      (> 0)
28	///   - k_at(i)   Winkler foundation modulus at node i [N/m^2] (>= 0; 0 = none)
29	///   - q_at(i)   distributed transverse load at node i [N/m]
30	/// plus optional applied actions at free ends (force [N] and moment [N*m]).
31	class Beam {
32	public:
33	    /// Construct a beam of length `length` [m] with a uniform flexural rigidity
34	    /// `EI` [N*m^2], discretized into `num_intervals` equal cells, with the
35	    /// given end supports. EI(x) is initialised constant, k(x) = 0, q(x) = 0.
36	    /// Throws std::invalid_argument if length or EI is non-positive or
37	    /// num_intervals < 2.
38	    Beam(double length, double EI, std::size_t num_intervals, Support left,
39	         Support right);
40	
41	    // ---- Field setters -------------------------------------------------------
42	
43	    /// Set the nodal flexural-rigidity field EI(x_i). Size must equal
44	    /// num_nodes(); every value must be > 0. Throws std::invalid_argument.
45	    void set_ei_nodal(const std::vector<double>& ei);
46	
47	    /// Set EI(x) from piecewise-linear control points (x, value), sampled at
48	    /// each node. Points are taken in the given order; x outside the range is
49	    /// clamped to the nearest endpoint value. Every sampled value must be > 0.
50	    void set_ei_profile(const std::vector<std::pair<double, double>>& points);
51	
52	    /// Set the nodal Winkler foundation field k(x_i) >= 0. Size == num_nodes().
53	    void set_foundation_nodal(const std::vector<double>& k);
54	
55	    /// Set k(x) from piecewise-linear control points (x, value).
56	    void set_foundation_profile(
57	        const std::vector<std::pair<double, double>>& points);
58	
59	    /// Set the nodal distributed-load field q(x_i). Size == num_nodes().
60	    void set_q_nodal(const std::vector<double>& q);
61	
62	    /// Set a uniform distributed load q [N/m] over the whole span (overwrites
63	    /// the load field).
64	    void set_distributed_load(double q);
65	
66	    /// Add a piecewise-linear distributed-load segment ramping from q0 at x0 to
67	    /// q1 at x1 [N/m] to the existing load field. Segments are additive.
68	    void add_load_segment(double x0, double x1, double q0, double q1);
69	
70	    /// Apply a transverse force P [N] at a free end (`at_left_end` -> x = 0,
71	    /// else x = L). Throws std::runtime_error if that end is not Free.
72	    void set_end_load(double P, bool at_left_end);
73	
74	    /// Apply a concentrated moment M [N*m] at a free end. Throws
75	    /// std::runtime_error if that end is not Free.
76	    void set_end_moment(double M, bool at_left_end);
77	
78	    // ---- Accessors -----------------------------------------------------------
79	
80	    double length() const { return length_; }
81	    std::size_t num_intervals() const { return num_intervals_; }
82	    std::size_t num_nodes() const { return num_intervals_ + 1; }
83	    double dx() const { return length_ / static_cast<double>(num_intervals_); }
84	    double node_x(std::size_t i) const;
85	
86	    Support left() const { return left_; }
87	    Support right() const { return right_; }
88	
89	    double EI_at(std::size_t i) const;  ///< nodal flexural rigidity [N*m^2]
90	    double k_at(std::size_t i) const;   ///< nodal foundation modulus [N/m^2]
91	    double q_at(std::size_t i) const;   ///< nodal distributed load [N/m]
92	
93	    /// A representative (maximum nodal) flexural rigidity [N*m^2], used as a
94	    /// scale for residual normalisation. Equals the constant EI for a uniform
95	    /// beam.
96	    double EI() const;
97	
98	    /// True if any nodal foundation modulus is strictly positive.
99	    bool has_foundation() const;
100	
101	    /// Applied end shear V at a free end (`left_end` -> x = 0). A transverse
102	    /// force P at a free end contributes V = -P; 0 if no force is applied.
103	    double applied_end_shear(bool left_end) const;
104	
105	    /// Applied end moment M [N*m] at a free end (0 if none).
106	    double end_moment(bool left_end) const;
107	
108	    /// True if any end force has been applied.
109	    bool has_end_load() const;
110	
111	    /// Throws std::runtime_error if the support / foundation combination cannot
112	    /// suppress rigid-body motion (a free end opposite a non-clamped end, or
113	    /// two free ends, is a mechanism UNLESS an elastic foundation is present).
114	    void validate() const;
115	
116	private:
117	    static std::size_t end_index(bool left_end) { return left_end ? 0u : 1u; }
118	
119	    double length_{0.0};
120	    std::size_t num_intervals_{0};
121	    Support left_{Support::Clamped};
122	    Support right_{Support::Free};
123	    std::vector<double> ei_;  // nodal EI, length num_nodes()
124	    std::vector<double> k_;   // nodal foundation, length num_nodes()
125	    std::vector<double> q_;   // nodal load, length num_nodes()
126	    double force_[2]{0.0, 0.0};   // applied transverse force [left, right]
127	    double moment_[2]{0.0, 0.0};  // applied moment [left, right]
128	};
129	
130	} // namespace beamfd
131	
132	#endif // BEAMFD_BEAM_HPP
133

/opt/beamfd/include/beamfd/linalg.hpp

contents
1	#ifndef BEAMFD_LINALG_HPP
2	#define BEAMFD_LINALG_HPP
3	
4	#include <cstddef>
5	#include <stdexcept>
6	#include <vector>
7	
8	namespace beamfd {
9	
10	/// A small, row-major dense matrix of doubles.
11	///
12	/// Part of the engine's linear-algebra support layer; fully implemented. The
13	/// beam solver uses it to hold the finite-difference system matrix A in
14	/// A w = b. Unlike a structural stiffness matrix, A here is generally NON
15	/// symmetric (boundary-condition rows are one-sided difference stencils), so
16	/// the solve uses a general LU factorization rather than a Cholesky/LDL^T.
17	class DenseMatrix {
18	public:
19	    DenseMatrix() = default;
20	
21	    DenseMatrix(std::size_t rows, std::size_t cols)
22	        : rows_(rows), cols_(cols), data_(rows * cols, 0.0) {}
23	
24	    std::size_t rows() const { return rows_; }
25	    std::size_t cols() const { return cols_; }
26	
27	    double& operator()(std::size_t r, std::size_t c) {
28	        return data_[r * cols_ + c];
29	    }
30	    double operator()(std::size_t r, std::size_t c) const {
31	        return data_[r * cols_ + c];
32	    }
33	
34	    void fill(double v) {
35	        for (auto& x : data_) x = v;
36	    }
37	
38	private:
39	    std::size_t rows_{0};
40	    std::size_t cols_{0};
41	    std::vector<double> data_;
42	};
43	
44	/// Solve the general (possibly non-symmetric) linear system A x = b by LU
45	/// factorization with partial (row) pivoting.
46	///
47	/// `A` is the n-by-n system matrix and `b` is the right-hand side of length n.
48	/// Returns the solution vector x of length n.
49	///
50	/// Throws std::runtime_error if A is not square, if the dimensions are
51	/// inconsistent, or if A is detected to be singular (a pivot column is
52	/// numerically zero), which is how an under-/over-determined boundary-value
53	/// problem surfaces.
54	std::vector<double> solve_general(const DenseMatrix& A,
55	                                  const std::vector<double>& b);
56	
57	} // namespace beamfd
58	
59	#endif // BEAMFD_LINALG_HPP
60

/opt/beamfd/include/beamfd/types.hpp

contents
1	#ifndef BEAMFD_TYPES_HPP
2	#define BEAMFD_TYPES_HPP
3	
4	#include <cstddef>
5	
6	namespace beamfd {
7	
8	/// Type of support condition applied at one end of the beam.
9	///
10	///  - Clamped (built-in / fixed): deflection and slope are both zero
11	///    (w = 0, w' = 0).
12	///  - Pinned (simple support):    deflection is zero and the bending moment
13	///    is zero (w = 0, M = 0).
14	///  - Free:                       the bending moment and shear take their
15	///    applied values (M = M_applied, V = V_applied), both zero when no end
16	///    action is applied.
17	///
18	/// See instruction.md for the continuum boundary-value problem these encode.
19	enum class Support {
20	    Clamped,
21	    Pinned,
22	    Free,
23	};
24	
25	} // namespace beamfd
26	
27	#endif // BEAMFD_TYPES_HPP
28
Let me check the Beam implementation for sign conventions and the existing test.
shell
find . -name '*.cpp' -o -name '*.beam' -o -name 'CMakeLists.txt' | head -50; echo "---TESTS---"; ls tests 2>/dev/null
output
./CMakeLists.txt
./examples/cantilever_tip.beam
./src/beam.cpp
./src/io.cpp
./src/linalg.cpp
./src/main.cpp
./src/solver.cpp
./tests/CMakeLists.txt
./tests/test_smoke.cpp
---TESTS---
CMakeLists.txt
test_smoke.cpp
test_util.hpp

[stdout]
./CMakeLists.txt
./examples/cantilever_tip.beam
./src/beam.cpp
./src/io.cpp
./src/linalg.cpp
./src/main.cpp
./src/solver.cpp
./tests/CMakeLists.txt
./tests/test_smoke.cpp
---TESTS---
CMakeLists.txt
test_smoke.cpp
test_util.hpp

/opt/beamfd/src/beam.cpp

contents
1	#include "beamfd/beam.hpp"
2	
3	#include <algorithm>
4	#include <stdexcept>
5	
6	namespace beamfd {
7	
8	namespace {
9	
10	// Piecewise-linear interpolation of control points (x, value) at coordinate x.
11	// Points are used in the given order (assumed nondecreasing in x); x outside
12	// the range is clamped to the nearest endpoint.
13	double interp(const std::vector<std::pair<double, double>>& pts, double x) {
14	    if (pts.empty()) {
15	        throw std::invalid_argument("Beam: empty profile control points");
16	    }
17	    if (x <= pts.front().first) return pts.front().second;
18	    if (x >= pts.back().first) return pts.back().second;
19	    for (std::size_t s = 1; s < pts.size(); ++s) {
20	        const double x0 = pts[s - 1].first, x1 = pts[s].first;
21	        if (x <= x1) {
22	            const double t = (x1 > x0) ? (x - x0) / (x1 - x0) : 0.0;
23	            return pts[s - 1].second + t * (pts[s].second - pts[s - 1].second);
24	        }
25	    }
26	    return pts.back().second;
27	}
28	
29	} // namespace
30	
31	Beam::Beam(double length, double EI, std::size_t num_intervals, Support left,
32	           Support right)
33	    : length_(length),
34	      num_intervals_(num_intervals),
35	      left_(left),
36	      right_(right) {
37	    if (length_ <= 0.0) {
38	        throw std::invalid_argument("Beam: length must be positive");
39	    }
40	    if (EI <= 0.0) {
41	        throw std::invalid_argument("Beam: EI must be positive");
42	    }
43	    if (num_intervals_ < 2) {
44	        throw std::invalid_argument("Beam: need at least 2 intervals");
45	    }
46	    const std::size_t n = num_nodes();
47	    ei_.assign(n, EI);
48	    k_.assign(n, 0.0);
49	    q_.assign(n, 0.0);
50	}
51	
52	void Beam::set_ei_nodal(const std::vector<double>& ei) {
53	    if (ei.size() != num_nodes()) {
54	        throw std::invalid_argument("Beam::set_ei_nodal: size mismatch");
55	    }
56	    for (double v : ei) {
57	        if (v <= 0.0) {
58	            throw std::invalid_argument("Beam::set_ei_nodal: EI must be positive");
59	        }
60	    }
61	    ei_ = ei;
62	}
63	
64	void Beam::set_ei_profile(const std::vector<std::pair<double, double>>& points) {
65	    std::vector<double> ei(num_nodes());
66	    for (std::size_t i = 0; i < num_nodes(); ++i) ei[i] = interp(points, node_x(i));
67	    set_ei_nodal(ei);
68	}
69	
70	void Beam::set_foundation_nodal(const std::vector<double>& k) {
71	    if (k.size() != num_nodes()) {
72	        throw std::invalid_argument("Beam::set_foundation_nodal: size mismatch");
73	    }
74	    for (double v : k) {
75	        if (v < 0.0) {
76	            throw std::invalid_argument(
77	                "Beam::set_foundation_nodal: k must be non-negative");
78	        }
79	    }
80	    k_ = k;
81	}
82	
83	void Beam::set_foundation_profile(
84	    const std::vector<std::pair<double, double>>& points) {
85	    std::vector<double> k(num_nodes());
86	    for (std::size_t i = 0; i < num_nodes(); ++i) k[i] = interp(points, node_x(i));
87	    set_foundation_nodal(k);
88	}
89	
90	void Beam::set_q_nodal(const std::vector<double>& q) {
91	    if (q.size() != num_nodes()) {
92	        throw std::invalid_argument("Beam::set_q_nodal: size mismatch");
93	    }
94	    q_ = q;
95	}
96	
97	void Beam::set_distributed_load(double q) { q_.assign(num_nodes(), q); }
98	
99	void Beam::add_load_segment(double x0, double x1, double q0, double q1) {
100	    if (x1 < x0) {
101	        std::swap(x0, x1);
102	        std::swap(q0, q1);
103	    }
104	    for (std::size_t i = 0; i < num_nodes(); ++i) {
105	        const double x = node_x(i);
106	        if (x < x0 || x > x1) continue;
107	        const double t = (x1 > x0) ? (x - x0) / (x1 - x0) : 0.0;
108	        q_[i] += q0 + t * (q1 - q0);
109	    }
110	}
111	
112	void Beam::set_end_load(double P, bool at_left_end) {
113	    const Support s = at_left_end ? left_ : right_;
114	    if (s != Support::Free) {
115	        throw std::runtime_error(
116	            "Beam::set_end_load: end load may only be applied at a free end");
117	    }
118	    force_[end_index(at_left_end)] = P;
119	}
120	
121	void Beam::set_end_moment(double M, bool at_left_end) {
122	    const Support s = at_left_end ? left_ : right_;
123	    if (s != Support::Free) {
124	        throw std::runtime_error(
125	            "Beam::set_end_moment: end moment may only be applied at a free end");
126	    }
127	    moment_[end_index(at_left_end)] = M;
128	}
129	
130	double Beam::node_x(std::size_t i) const {
131	    if (i > num_intervals_) {
132	        throw std::out_of_range("Beam::node_x: node index out of range");
133	    }
134	    return static_cast<double>(i) * dx();
135	}
136	
137	double Beam::EI_at(std::size_t i) const {
138	    if (i >= ei_.size()) throw std::out_of_range("Beam::EI_at: index out of range");
139	    return ei_[i];
140	}
141	
142	double Beam::k_at(std::size_t i) const {
143	    if (i >= k_.size()) throw std::out_of_range("Beam::k_at: index out of range");
144	    return k_[i];
145	}
146	
147	double Beam::q_at(std::size_t i) const {
148	    if (i >= q_.size()) throw std::out_of_range("Beam::q_at: index out of range");
149	    return q_[i];
150	}
151	
152	double Beam::EI() const {
153	    double m = 0.0;
154	    for (double v : ei_) m = std::max(m, v);
155	    return m;
156	}
157	
158	bool Beam::has_foundation() const {
159	    for (double v : k_) {
160	        if (v > 0.0) return true;
161	    }
162	    return false;
163	}
164	
165	double Beam::applied_end_shear(bool left_end) const {
166	    return -force_[end_index(left_end)];
167	}
168	
169	double Beam::end_moment(bool left_end) const { return moment_[end_index(left_end)]; }
170	
171	bool Beam::has_end_load() const { return force_[0] != 0.0 || force_[1] != 0.0; }
172	
173	void Beam::validate() const {
174	    const bool left_free = (left_ == Support::Free);
175	    const bool right_free = (right_ == Support::Free);
176	
177	    // An elastic foundation supplies distributed restraint that removes the
178	    // rigid-body modes, so any support combination is well posed when present.
179	    if (has_foundation()) return;
180	
181	    if (left_free && right_free) {
182	        throw std::runtime_error("Beam::validate: free-free beam is a mechanism");
183	    }
184	    if (left_free && right_ != Support::Clamped) {
185	        throw std::runtime_error(
186	            "Beam::validate: a free end requires a clamped opposite end");
187	    }
188	    if (right_free && left_ != Support::Clamped) {
189	        throw std::runtime_error(
190	            "Beam::validate: a free end requires a clamped opposite end");
191	    }
192	}
193	
194	} // namespace beamfd
195
Let me look at the smoke test and the example to understand conventions and expected behavior.

/opt/beamfd/tests/test_smoke.cpp

contents
1	// Smoke test for the beamfd project: a minimal, non-leaky sanity check so the
2	// project compiles and a solver gets quick feedback. It asserts only generic
3	// properties (finite field, pinned ends fixed, a non-trivial deflection, and a
4	// small interior discrete-equilibrium residual) and contains NO closed-form
5	// answer. The authoritative grading is performed by a separate hidden suite.
6	
7	#include <algorithm>
8	#include <cmath>
9	
10	#include "beamfd/beam.hpp"
11	#include "beamfd/solver.hpp"
12	#include "test_util.hpp"
13	
14	using namespace beamfd;
15	
16	BEAMFD_TEST("smoke_pinned_udl_sane") {
17	    Beam beam(2.0, 1000.0, 20, Support::Pinned, Support::Pinned);
18	    beam.set_distributed_load(5.0);
19	    BeamSolver solver(beam);
20	    BeamResult r = solver.solve();
21	    const std::size_t n = beam.num_nodes();
22	
23	    beamfd_test::expect(r.deflection.size() == n, "deflection has num_nodes entries");
24	    for (double w : r.deflection) {
25	        beamfd_test::expect(std::isfinite(w), "deflection is finite");
26	    }
27	    beamfd_test::expect_near(r.deflection[0], 0.0, 1e-9, "left pin fixed");
28	    beamfd_test::expect_near(r.deflection[n - 1], 0.0, 1e-9, "right pin fixed");
29	    beamfd_test::expect(r.deflection[n / 2] > 0.0, "mid-span deflects under load");
30	
31	    // Interior discrete-equilibrium residual A w - b ~ 0 (relative to scale).
32	    BeamSystem sys = solver.assemble_system();
33	    double scale = 0.0;
34	    for (double w : r.deflection) scale = std::max(scale, std::fabs(w));
35	    const double c4 = beam.EI() / std::pow(beam.dx(), 4);
36	    for (std::size_t i = 2; i + 2 < n; ++i) {
37	        double res = -sys.b[i];
38	        for (std::size_t j = 0; j < n; ++j) res += sys.A(i, j) * r.deflection[j];
39	        beamfd_test::expect(std::fabs(res) <= 1e-6 * (c4 * scale) + 1e-9,
40	                            "interior equilibrium residual is small");
41	    }
42	}
43	
44	BEAMFD_TEST_MAIN()
45

/opt/beamfd/examples/cantilever_tip.beam

contents
1	# Cantilever beam with a downward point load at the free tip.
2	# Clamped (built-in) at x = 0, free at x = L.
3	length 3.0          # span [m]
4	ei     2.0e6        # flexural rigidity EI [N*m^2]
5	cells  200          # number of equal finite-difference intervals
6	
7	# Left end clamped, right end free.
8	support clamped free
9	
10	# Downward point load of 1 kN at the free right tip.
11	endload right 1000.0
12
I have a clear picture now. Key facts I've gathered: - Governing equation: `(EI w'')'' + k w = q`, conservative form. - The recovery helpers define the discrete `M_i = EI_i·w''_i` and `V_i = (EI w'')'_i` with specific one-sided stencils at the ends , I'll make my free-end BC rows match these exactly for consistency. - `linalg.hpp` confirms the intended design: **BC rows are one-sided difference stencils** (no ghost nodes). - The free-end RHS comes directly from `applied_end_shear(end)` / `end_moment(end)` , I follow that contract literally (it's self-consistent with how the grader manufactures solutions). - The smoke test checks interior equilibrium residual for rows `2..N-2`, confirming: rows 0,1 = left BCs, rows 2..N-2 = conservative ODE, rows N-1,N = right BCs. Let me write the implementation.

/opt/beamfd/src/solver.cpp

− removed
BeamSystem BeamSolver::assemble_system() const {
    // TODO(candidate): build and return the finite-difference system A w = b.
    const std::size_t n = beam_.num_nodes();
    BeamSystem sys;
    sys.A = DenseMatrix(n, n);  // all zeros -> singular / wrong
    sys.b.assign(n, 0.0);
    return sys;
}

BeamSystem BeamSolver::solve() const {
+ added
BeamSystem BeamSolver::assemble_system() const {
    // Uniform grid x_i = i*h, i = 0..N, with n = N+1 nodal unknowns w_i.
    //
    // Governing equation (conservative / divergence form):
    //
    //     d^2/dx^2 ( EI(x) w''(x) ) + k(x) w(x) = q(x)
    //
    // Discretization (second-order accurate):
    //   * Interior rows i = 2..N-2 enforce the conservative bending operator as
    //     the second difference of the nodal bending moment m_j = EI_j w''_j:
    //
    //         L_i = ( m_{i-1} - 2 m_i + m_{i+1} ) / h^2 ,
    //         m_j = EI_j ( w_{j-1} - 2 w_j + w_{j+1} ) / h^2 ,
    //
    //     giving a five-point stencil that reduces to the usual biharmonic
    //     stencil EI/h^4 * [1 -4 6 -4 1] when EI is constant. The discrete
    //     equation is L_i + k_i w_i = q_i.
    //   * The first/last two rows are the boundary conditions, written as
    //     one-sided difference stencils consistent to the same order. The
    //     natural (free-end) rows reuse exactly the discrete M and V operators
    //     of the recovery helpers, so the BC RHS are end_moment / applied_end_shear.
    const std::size_t n = beam_.num_nodes();
    const std::size_t N = beam_.num_intervals();  // n - 1
    const double h = beam_.dx();
    const double h2 = h * h;
    const double h4 = h2 * h2;

    BeamSystem sys;
    sys.A = DenseMatrix(n, n);
    sys.b.assign(n, 0.0);
    DenseMatrix& A = sys.A;
    std::vector<double>& b = sys.b;

    // ---- Interior conservative bending rows: i = 2 .. N-2 ------------------
    for (std::size_t i = 2; i + 2 <= N; ++i) {
        const double EIm = beam_.EI_at(i - 1);
        const double EIc = beam_.EI_at(i);
        const double EIp = beam_.EI_at(i + 1);
        A(i, i - 2) += EIm / h4;
        A(i, i - 1) += (-2.0 * EIm - 2.0 * EIc) / h4;
        A(i, i) += (EIm + 4.0 * EIc + EIp) / h4 + beam_.k_at(i);
        A(i, i + 1) += (-2.0 * EIc - 2.0 * EIp) / h4;
        A(i, i + 2) += EIp / h4;
        b[i] = beam_.q_at(i);
    }

    // ---- Left boundary conditions: rows 0 and 1 ---------------------------
    switch (beam_.left()) {
        case Support::Clamped: {
            // w(0) = 0
            A(0, 0) = 1.0;
            b[0] = 0.0;
            // w'(0) = 0 via second-order forward difference.
            A(1, 0) = -3.0 / (2.0 * h);
            A(1, 1) = 4.0 / (2.0 * h);
            A(1, 2) = -1.0 / (2.0 * h);
            b[1] = 0.0;
            break;
        }
        case Support::Pinned: {
            // w(0) = 0
            A(0, 0) = 1.0;
            b[0] = 0.0;
            // M(0) = EI w''(0) = 0; one-sided second derivative (scaled to O(1)).
            A(1, 0) = 2.0;
            A(1, 1) = -5.0;
            A(1, 2) = 4.0;
            A(1, 3) = -1.0;
            b[1] = 0.0;
            break;
        }
        case Support::Free: {
            const double EI0 = beam_.EI_at(0);
            const double EI1 = beam_.EI_at(1);
            const double EI2 = beam_.EI_at(2);
            // Row 0: M(0) = EI0 * (2 w0 - 5 w1 + 4 w2 - w3)/h^2 = end_moment.
            A(0, 0) = EI0 * 2.0 / h2;
            A(0, 1) = EI0 * -5.0 / h2;
            A(0, 2) = EI0 * 4.0 / h2;
            A(0, 3) = EI0 * -1.0 / h2;
            b[0] = beam_.end_moment(true);
            // Row 1: V(0) = (-3 m0 + 4 m1 - m2)/(2h) = applied_end_shear, with
            //   m0 = EI0 (2 w0 - 5 w1 + 4 w2 - w3)/h^2  (one-sided)
            //   m1 = EI1 (w0 - 2 w1 + w2)/h^2           (central)
            //   m2 = EI2 (w1 - 2 w2 + w3)/h^2           (central)
            const double c = 1.0 / (2.0 * h * h2);
            A(1, 0) += c * (-3.0 * EI0 * 2.0 + 4.0 * EI1 * 1.0);
            A(1, 1) += c * (-3.0 * EI0 * -5.0 + 4.0 * EI1 * -2.0 - 1.0 * EI2 * 1.0);
            A(1, 2) += c * (-3.0 * EI0 * 4.0 + 4.0 * EI1 * 1.0 - 1.0 * EI2 * -2.0);
            A(1, 3) += c * (-3.0 * EI0 * -1.0 - 1.0 * EI2 * 1.0);
            b[1] = beam_.applied_end_shear(true);
            break;
        }
    }

    // ---- Right boundary conditions: rows N-1 and N ------------------------
    switch (beam_.right()) {
        case Support::Clamped: {
            // w(L) = 0
            A(N, N) = 1.0;
            b[N] = 0.0;
            // w'(L) = 0 via second-order backward difference.
            A(N - 1, N) = 3.0 / (2.0 * h);
            A(N - 1, N - 1) = -4.0 / (2.0 * h);
            A(N - 1, N - 2) = 1.0 / (2.0 * h);
            b[N - 1] = 0.0;
            break;
        }
        case Support::Pinned: {
            // w(L) = 0
            A(N, N) = 1.0;
            b[N] = 0.0;
            // M(L) = EI w''(L) = 0; one-sided second derivative (scaled to O(1)).
            A(N - 1, N) = 2.0;
            A(N - 1, N - 1) = -5.0;
            A(N - 1, N - 2) = 4.0;
            A(N - 1, N - 3) = -1.0;
            b[N - 1] = 0.0;
            break;
        }
        case Support::Free: {
            const double EIN = beam_.EI_at(N);
            const double EINm1 = beam_.EI_at(N - 1);
            const double EINm2 = beam_.EI_at(N - 2);
            // Row N: M(L) = EIN * (2 wN - 5 w_{N-1} + 4 w_{N-2} - w_{N-3})/h^2.
            A(N, N) = EIN * 2.0 / h2;
            A(N, N - 1) = EIN * -5.0 / h2;
            A(N, N - 2) = EIN * 4.0 / h2;
            A(N, N - 3) = EIN * -1.0 / h2;
            b[N] = beam_.end_moment(false);
            // Row N-1: V(L) = (3 mN - 4 m_{N-1} + m_{N-2})/(2h), with
            //   mN     = EIN   (2 wN - 5 w_{N-1} + 4 w_{N-2} - w_{N-3})/h^2
            //   m_{N-1}= EINm1 (w_{N-2} - 2 w_{N-1} + wN)/h^2
            //   m_{N-2}= EINm2 (w_{N-3} - 2 w_{N-2} + w_{N-1})/h^2
            const double c = 1.0 / (2.0 * h * h2);
            A(N - 1, N) += c * (3.0 * EIN * 2.0 - 4.0 * EINm1 * 1.0);
            A(N - 1, N - 1) +=
                c * (3.0 * EIN * -5.0 - 4.0 * EINm1 * -2.0 + 1.0 * EINm2 * 1.0);
            A(N - 1, N - 2) +=
                c * (3.0 * EIN * 4.0 - 4.0 * EINm1 * 1.0 + 1.0 * EINm2 * -2.0);
            A(N - 1, N - 3) += c * (3.0 * EIN * -1.0 + 1.0 * EINm2 * 1.0);
            b[N - 1] = beam_.applied_end_shear(false);
            break;
        }
    }

    return sys;
}

BeamResult BeamSolver::solve() const {
I mistyped the return type in my anchor. Let me fix the two functions separately.

/opt/beamfd/src/solver.cpp

− removed
BeamSystem BeamSolver::assemble_system() const {
    // TODO(candidate): build and return the finite-difference system A w = b.
    const std::size_t n = beam_.num_nodes();
    BeamSystem sys;
    sys.A = DenseMatrix(n, n);  // all zeros -> singular / wrong
    sys.b.assign(n, 0.0);
    return sys;
}

BeamResult BeamSolver::solve() const {
    // TODO(candidate): validate, assemble, solve, return the deflection field.
    const std::size_t n = beam_.num_nodes();
    BeamResult result;
    result.deflection.assign(n, 0.0);  // trivially zero -> wrong
    return result;
}
+ added
BeamSystem BeamSolver::assemble_system() const {
    // Uniform grid x_i = i*h, i = 0..N, with n = N+1 nodal unknowns w_i.
    //
    // Governing equation (conservative / divergence form):
    //
    //     d^2/dx^2 ( EI(x) w''(x) ) + k(x) w(x) = q(x)
    //
    // Discretization (second-order accurate):
    //   * Interior rows i = 2..N-2 enforce the conservative bending operator as
    //     the second difference of the nodal bending moment m_j = EI_j w''_j:
    //
    //         L_i = ( m_{i-1} - 2 m_i + m_{i+1} ) / h^2 ,
    //         m_j = EI_j ( w_{j-1} - 2 w_j + w_{j+1} ) / h^2 ,
    //
    //     giving a five-point stencil that reduces to the usual biharmonic
    //     stencil EI/h^4 * [1 -4 6 -4 1] when EI is constant. The discrete
    //     equation is L_i + k_i w_i = q_i.
    //   * The first/last two rows are the boundary conditions, written as
    //     one-sided difference stencils consistent to the same order. The
    //     natural (free-end) rows reuse exactly the discrete M and V operators
    //     of the recovery helpers, so their RHS are end_moment / applied_end_shear.
    const std::size_t n = beam_.num_nodes();
    const std::size_t N = beam_.num_intervals();  // n - 1
    const double h = beam_.dx();
    const double h2 = h * h;
    const double h4 = h2 * h2;

    BeamSystem sys;
    sys.A = DenseMatrix(n, n);
    sys.b.assign(n, 0.0);
    DenseMatrix& A = sys.A;
    std::vector<double>& b = sys.b;

    // ---- Interior conservative bending rows: i = 2 .. N-2 ------------------
    for (std::size_t i = 2; i + 2 <= N; ++i) {
        const double EIm = beam_.EI_at(i - 1);
        const double EIc = beam_.EI_at(i);
        const double EIp = beam_.EI_at(i + 1);
        A(i, i - 2) += EIm / h4;
        A(i, i - 1) += (-2.0 * EIm - 2.0 * EIc) / h4;
        A(i, i) += (EIm + 4.0 * EIc + EIp) / h4 + beam_.k_at(i);
        A(i, i + 1) += (-2.0 * EIc - 2.0 * EIp) / h4;
        A(i, i + 2) += EIp / h4;
        b[i] = beam_.q_at(i);
    }

    // ---- Left boundary conditions: rows 0 and 1 ---------------------------
    switch (beam_.left()) {
        case Support::Clamped: {
            // w(0) = 0
            A(0, 0) = 1.0;
            b[0] = 0.0;
            // w'(0) = 0 via second-order forward difference.
            A(1, 0) = -3.0 / (2.0 * h);
            A(1, 1) = 4.0 / (2.0 * h);
            A(1, 2) = -1.0 / (2.0 * h);
            b[1] = 0.0;
            break;
        }
        case Support::Pinned: {
            // w(0) = 0
            A(0, 0) = 1.0;
            b[0] = 0.0;
            // M(0) = EI w''(0) = 0; one-sided second derivative (scaled to O(1)).
            A(1, 0) = 2.0;
            A(1, 1) = -5.0;
            A(1, 2) = 4.0;
            A(1, 3) = -1.0;
            b[1] = 0.0;
            break;
        }
        case Support::Free: {
            const double EI0 = beam_.EI_at(0);
            const double EI1 = beam_.EI_at(1);
            const double EI2 = beam_.EI_at(2);
            // Row 0: M(0) = EI0 * (2 w0 - 5 w1 + 4 w2 - w3)/h^2 = end_moment.
            A(0, 0) = EI0 * 2.0 / h2;
            A(0, 1) = EI0 * -5.0 / h2;
            A(0, 2) = EI0 * 4.0 / h2;
            A(0, 3) = EI0 * -1.0 / h2;
            b[0] = beam_.end_moment(true);
            // Row 1: V(0) = (-3 m0 + 4 m1 - m2)/(2h) = applied_end_shear, with
            //   m0 = EI0 (2 w0 - 5 w1 + 4 w2 - w3)/h^2  (one-sided)
            //   m1 = EI1 (w0 - 2 w1 + w2)/h^2           (central)
            //   m2 = EI2 (w1 - 2 w2 + w3)/h^2           (central)
            const double c = 1.0 / (2.0 * h * h2);
            A(1, 0) += c * (-3.0 * EI0 * 2.0 + 4.0 * EI1 * 1.0);
            A(1, 1) += c * (-3.0 * EI0 * -5.0 + 4.0 * EI1 * -2.0 - 1.0 * EI2 * 1.0);
            A(1, 2) += c * (-3.0 * EI0 * 4.0 + 4.0 * EI1 * 1.0 - 1.0 * EI2 * -2.0);
            A(1, 3) += c * (-3.0 * EI0 * -1.0 - 1.0 * EI2 * 1.0);
            b[1] = beam_.applied_end_shear(true);
            break;
        }
    }

    // ---- Right boundary conditions: rows N-1 and N ------------------------
    switch (beam_.right()) {
        case Support::Clamped: {
            // w(L) = 0
            A(N, N) = 1.0;
            b[N] = 0.0;
            // w'(L) = 0 via second-order backward difference.
            A(N - 1, N) = 3.0 / (2.0 * h);
            A(N - 1, N - 1) = -4.0 / (2.0 * h);
            A(N - 1, N - 2) = 1.0 / (2.0 * h);
            b[N - 1] = 0.0;
            break;
        }
        case Support::Pinned: {
            // w(L) = 0
            A(N, N) = 1.0;
            b[N] = 0.0;
            // M(L) = EI w''(L) = 0; one-sided second derivative (scaled to O(1)).
            A(N - 1, N) = 2.0;
            A(N - 1, N - 1) = -5.0;
            A(N - 1, N - 2) = 4.0;
            A(N - 1, N - 3) = -1.0;
            b[N - 1] = 0.0;
            break;
        }
        case Support::Free: {
            const double EIN = beam_.EI_at(N);
            const double EINm1 = beam_.EI_at(N - 1);
            const double EINm2 = beam_.EI_at(N - 2);
            // Row N: M(L) = EIN * (2 wN - 5 w_{N-1} + 4 w_{N-2} - w_{N-3})/h^2.
            A(N, N) = EIN * 2.0 / h2;
            A(N, N - 1) = EIN * -5.0 / h2;
            A(N, N - 2) = EIN * 4.0 / h2;
            A(N, N - 3) = EIN * -1.0 / h2;
            b[N] = beam_.end_moment(false);
            // Row N-1: V(L) = (3 mN - 4 m_{N-1} + m_{N-2})/(2h), with
            //   mN     = EIN   (2 wN - 5 w_{N-1} + 4 w_{N-2} - w_{N-3})/h^2
            //   m_{N-1}= EINm1 (w_{N-2} - 2 w_{N-1} + wN)/h^2
            //   m_{N-2}= EINm2 (w_{N-3} - 2 w_{N-2} + w_{N-1})/h^2
            const double c = 1.0 / (2.0 * h * h2);
            A(N - 1, N) += c * (3.0 * EIN * 2.0 - 4.0 * EINm1 * 1.0);
            A(N - 1, N - 1) +=
                c * (3.0 * EIN * -5.0 - 4.0 * EINm1 * -2.0 + 1.0 * EINm2 * 1.0);
            A(N - 1, N - 2) +=
                c * (3.0 * EIN * 4.0 - 4.0 * EINm1 * 1.0 + 1.0 * EINm2 * -2.0);
            A(N - 1, N - 3) += c * (3.0 * EIN * -1.0 + 1.0 * EINm2 * 1.0);
            b[N - 1] = beam_.applied_end_shear(false);
            break;
        }
    }

    return sys;
}

BeamResult BeamSolver::solve() const {
    // Validate the support/foundation configuration first; let mechanism errors
    // propagate. Then assemble and solve A w = b (a singular system surfaces as
    // an exception from solve_general, which also propagates).
    beam_.validate();
    const BeamSystem sys = assemble_system();
    BeamResult result;
    result.deflection = solve_general(sys.A, sys.b);
    return result;
}
Now let me build and test.
shell
cmake -S . -B build -DCMAKE_BUILD_TYPE=Release >/tmp/cm.log 2>&1 && cmake --build build --parallel >/tmp/build.log 2>&1 && echo BUILD_OK && cd build && ctest --output-on-failure 2>&1 | tail -20
output
BUILD_OK
Test project /opt/beamfd/build
    Start 1: smoke
1/1 Test #1: smoke ............................   Passed    0.00 sec

100% tests passed, 0 tests failed out of 1

Total Test time (real) =   0.01 sec

[stdout]
BUILD_OK
Test project /opt/beamfd/build
    Start 1: smoke
1/1 Test #1: smoke ............................   Passed    0.00 sec

100% tests passed, 0 tests failed out of 1

Total Test time (real) =   0.01 sec
Smoke passes. Now let me independently verify accuracy and second-order convergence against manufactured solutions, since the hidden suite is the real grader. Let me check the build structure first.

/opt/beamfd/CMakeLists.txt

contents
1	cmake_minimum_required(VERSION 3.16)
2	project(beamfd LANGUAGES CXX)
3	
4	set(CMAKE_CXX_STANDARD 17)
5	set(CMAKE_CXX_STANDARD_REQUIRED ON)
6	set(CMAKE_CXX_EXTENSIONS OFF)
7	
8	if(NOT CMAKE_BUILD_TYPE)
9	  set(CMAKE_BUILD_TYPE Release)
10	endif()
11	
12	add_compile_options(-Wall -Wextra)
13	
14	# --- Core library -----------------------------------------------------------
15	add_library(beamfd
16	  src/linalg.cpp
17	  src/beam.cpp
18	  src/solver.cpp
19	  src/io.cpp
20	)
21	target_include_directories(beamfd PUBLIC ${CMAKE_CURRENT_SOURCE_DIR}/include)
22	
23	# --- Demo CLI ---------------------------------------------------------------
24	add_executable(beamfd_cli src/main.cpp)
25	target_link_libraries(beamfd_cli PRIVATE beamfd)
26	
27	# --- Tests ------------------------------------------------------------------
28	enable_testing()
29	add_subdirectory(tests)
30
shell
ls build; echo ---; ls build/*.a 2>/dev/null; find build -name '*.a' 2>/dev/null
output
ls: cannot access 'build': No such file or directory
---

[stdout]
ls: cannot access 'build': No such file or directory
---
shell
find /opt/beamfd/build -name '*.a' 2>/dev/null
output
/opt/beamfd/build/libbeamfd.a

[stdout]
/opt/beamfd/build/libbeamfd.a
Now let me write a comprehensive verification harness with manufactured solutions and convergence checks.
write · /opt/beamfd/verify.cpp
#include <cmath>
#include <cstdio>
#include <functional>
#include <vector>

#include "beamfd/beam.hpp"
#include "beamfd/solver.hpp"

using namespace beamfd;

static double max_err(const std::vector<double>& w,
                      const std::function<double(double)>& exact, const Beam& b) {
    double e = 0.0;
    for (std::size_t i = 0; i < w.size(); ++i)
        e = std::max(e, std::fabs(w[i] - exact(b.node_x(i))));
    return e;
}

static void order(const char* name, double e1, double e2) {
    // mesh doubled -> expect ratio ~4 for 2nd order
    printf("%-34s err(N)=%.3e err(2N)=%.3e ratio=%.2f order=%.2f\n", name, e1, e2,
           e1 / e2, std::log2(e1 / e2));
}

int main() {
    const double L = 3.0, EI = 2.0e6;

    // 1) Pinned-pinned, UDL q -> w = q x (L^3 - 2 L x^2 + x^3)/(24 EI)
    {
        const double q = 500.0;
        auto exact = [&](double x) {
            return q * x * (L * L * L - 2 * L * x * x + x * x * x) / (24 * EI);
        };
        auto run = [&](std::size_t N) {
            Beam b(L, EI, N, Support::Pinned, Support::Pinned);
            b.set_distributed_load(q);
            return max_err(BeamSolver(b).solve().deflection, exact, b);
        };
        order("pinned-pinned UDL", run(40), run(80));
    }

    // 2) Cantilever clamped-free, tip load P -> w = P x^2 (3L - x)/(6 EI)
    {
        const double P = 1000.0;
        auto exact = [&](double x) { return P * x * x * (3 * L - x) / (6 * EI); };
        auto run = [&](std::size_t N) {
            Beam b(L, EI, N, Support::Clamped, Support::Free);
            b.set_end_load(P, false);  // downward at right tip
            return max_err(BeamSolver(b).solve().deflection, exact, b);
        };
        order("cantilever tip load", run(40), run(80));
    }

    // 3) Cantilever clamped-free, tip moment M0 -> w = M0 x^2/(2 EI)
    {
        const double M0 = 1500.0;
        auto exact = [&](double x) { return M0 * x * x / (2 * EI); };
        auto run = [&](std::size_t N) {
            Beam b(L, EI, N, Support::Clamped, Support::Free);
            b.set_end_moment(M0, false);
            return max_err(BeamSolver(b).solve().deflection, exact, b);
        };
        order("cantilever tip moment", run(40), run(80));
    }

    // 4) Clamped-clamped, UDL -> w = q x^2 (L-x)^2/(24 EI)
    {
        const double q = 800.0;
        auto exact = [&](double x) {
            return q * x * x * (L - x) * (L - x) / (24 * EI);
        };
        auto run = [&](std::size_t N) {
            Beam b(L, EI, N, Support::Clamped, Support::Clamped);
            b.set_distributed_load(q);
            return max_err(BeamSolver(b).solve().deflection, exact, b);
        };
        order("clamped-clamped UDL", run(40), run(80));
    }

    // 5) Manufactured solution with VARIABLE EI and FOUNDATION.
    //    Pick w(x) = sin(pi x / L) (vanishes & has zero 2nd deriv at ends ->
    //    pinned-pinned), EI(x) = EI0 (1 + 0.5 x/L), k(x) = k0 (1 + x/L).
    //    Then q(x) = (EI w'')'' + k w  computed analytically.
    {
        const double EI0 = 1.0e6, k0 = 3.0e4;
        const double pi = std::acos(-1.0);
        auto EIf = [&](double x) { return EI0 * (1.0 + 0.5 * x / L); };
        auto EIp = [&](double) { return EI0 * 0.5 / L; };       // EI'
        auto kf = [&](double x) { return k0 * (1.0 + x / L); };
        auto w = [&](double x) { return std::sin(pi * x / L); };
        auto w2 = [&](double x) {
            return -(pi / L) * (pi / L) * std::sin(pi * x / L);
        };
        auto w3 = [&](double x) {
            return -(pi / L) * (pi / L) * (pi / L) * std::cos(pi * x / L);
        };
        auto w4 = [&](double x) {
            double a = pi / L;
            return a * a * a * a * std::sin(pi * x / L);
        };
        // (EI w'')'' = EI'' w'' + 2 EI' w''' + EI w''''  (EI'' = 0)
        auto q = [&](double x) {
            return 2.0 * EIp(x) * w3(x) + EIf(x) * w4(x) + kf(x) * w(x);
        };
        auto run = [&](std::size_t N) {
            Beam b(L, EI0, N, Support::Pinned, Support::Pinned);
            std::vector<double> ei(N + 1), kk(N + 1), qq(N + 1);
            for (std::size_t i = 0; i <= N; ++i) {
                double x = b.node_x(i);
                ei[i] = EIf(x);
                kk[i] = kf(x);
                qq[i] = q(x);
            }
            b.set_ei_nodal(ei);
            b.set_foundation_nodal(kk);
            b.set_q_nodal(qq);
            return max_err(BeamSolver(b).solve().deflection, w, b);
        };
        order("variable-EI + foundation (MMS)", run(80), run(160));
    }

    // 6) Free-free on a foundation (well posed due to foundation), MMS with
    //    w(x)=cos(pi x/L) so w'(0)=w'(L)=0 but free ends need M,V matched.
    //    Use constant EI, constant k. q=(EI w'''')+k w; set end M=EI w''(end),
    //    end V=(EI w'')'(end)=EI w'''(end).
    {
        const double EIc = 1.5e6, k0 = 5.0e4;
        const double pi = std::acos(-1.0);
        auto w = [&](double x) { return std::cos(pi * x / L); };
        auto w2 = [&](double x) {
            return -(pi / L) * (pi / L) * std::cos(pi * x / L);
        };
        auto w3 = [&](double x) {
            return (pi / L) * (pi / L) * (pi / L) * std::sin(pi * x / L);
        };
        auto w4 = [&](double x) {
            double a = pi / L;
            return a * a * a * a * std::cos(pi * x / L);
        };
        auto run = [&](std::size_t N) {
            Beam b(L, EIc, N, Support::Free, Support::Free);
            b.set_foundation_nodal(std::vector<double>(N + 1, k0));
            std::vector<double> qq(N + 1);
            for (std::size_t i = 0; i <= N; ++i) {
                double x = b.node_x(i);
                qq[i] = EIc * w4(x) + k0 * w(x);
            }
            b.set_q_nodal(qq);
            // End actions: M = EI w''(end); applied_end_shear = (EI w'')'(end).
            // set_end_moment sets end_moment(); set_end_load sets P with
            // applied_end_shear = -P, so P = -(EI w''')(end).
            b.set_end_moment(EIc * w2(0.0), true);
            b.set_end_moment(EIc * w2(L), false);
            b.set_end_load(-(EIc * w3(0.0)), true);
            b.set_end_load(-(EIc * w3(L)), false);
            return max_err(BeamSolver(b).solve().deflection, w, b);
        };
        order("free-free on foundation (MMS)", run(80), run(160));
    }

    return 0;
}
shell
cd /opt/beamfd && g++ -std=c++17 -O2 -Iinclude verify.cpp build/libbeamfd.a -o build/verify 2>&1 | head && ./build/verify
output
pinned-pinned UDL                  err(N)=1.450e-06 err(2N)=3.625e-07 ratio=4.00 order=2.00
cantilever tip load                err(N)=2.813e-06 err(2N)=7.031e-07 ratio=4.00 order=2.00
cantilever tip moment              err(N)=2.006e-13 err(2N)=3.709e-12 ratio=0.05 order=-4.21
clamped-clamped UDL                err(N)=8.121e-07 err(2N)=2.070e-07 ratio=3.92 order=1.97
variable-EI + foundation (MMS)     err(N)=1.767e-04 err(2N)=5.323e-05 ratio=3.32 order=1.73
free-free on foundation (MMS)      err(N)=4.473e+00 err(2N)=2.131e+00 ratio=2.10 order=1.07

[stdout]
pinned-pinned UDL                  err(N)=1.450e-06 err(2N)=3.625e-07 ratio=4.00 order=2.00
cantilever tip load                err(N)=2.813e-06 err(2N)=7.031e-07 ratio=4.00 order=2.00
cantilever tip moment              err(N)=2.006e-13 err(2N)=3.709e-12 ratio=0.05 order=-4.21
clamped-clamped UDL                err(N)=8.121e-07 err(2N)=2.070e-07 ratio=3.92 order=1.97
variable-EI + foundation (MMS)     err(N)=1.767e-04 err(2N)=5.323e-05 ratio=3.32 order=1.73
free-free on foundation (MMS)      err(N)=4.473e+00 err(2N)=2.131e+00 ratio=2.10 order=1.07
Excellent , this surfaced a real bug. The convergence results show: - Pinned/clamped/cantilever cases: clean **2nd order** ✓ - Tip moment: exact to round-off ✓ - **free-free on foundation: only order 1.07 with huge error** ✗ The issue: my free-end **shear** BC mixed a one-sided 2nd-derivative (for `m0`) with central ones (for `m1,m2`). Their differing leading error terms don't cancel under the first-difference, collapsing the composite to the forward 3rd-difference `(-1,3,-3,1)/h³`, which is only **first-order** for `w'''`. It looked clean for cubic solutions (cantilever) because the 3rd-difference is exact for cubics, but a curved solution exposes it. Let me fix the free-end shear rows with a proper 2nd-order one-sided stencil via the product rule `V = EI'·w'' + EI·w'''`, using the O(h²) one-sided third-derivative stencil.

/opt/beamfd/src/solver.cpp

− removed
            b[0] = beam_.end_moment(true);
            // Row 1: V(0) = (-3 m0 + 4 m1 - m2)/(2h) = applied_end_shear, with
            //   m0 = EI0 (2 w0 - 5 w1 + 4 w2 - w3)/h^2  (one-sided)
            //   m1 = EI1 (w0 - 2 w1 + w2)/h^2           (central)
            //   m2 = EI2 (w1 - 2 w2 + w3)/h^2           (central)
            const double c = 1.0 / (2.0 * h * h2);
            A(1, 0) += c * (-3.0 * EI0 * 2.0 + 4.0 * EI1 * 1.0);
            A(1, 1) += c * (-3.0 * EI0 * -5.0 + 4.0 * EI1 * -2.0 - 1.0 * EI2 * 1.0);
            A(1, 2) += c * (-3.0 * EI0 * 4.0 + 4.0 * EI1 * 1.0 - 1.0 * EI2 * -2.0);
            A(1, 3) += c * (-3.0 * EI0 * -1.0 - 1.0 * EI2 * 1.0);
            b[1] = beam_.applied_end_shear(true);
+ added
            b[0] = beam_.end_moment(true);
            // Row 1: V(0) = (EI w'')'(0) = EI'(0) w''(0) + EI(0) w'''(0), each
            // factor a second-order one-sided difference (product rule keeps the
            // whole shear operator O(h^2), unlike a composite nodal-moment form):
            //   EI'(0) ~ (-3 EI0 + 4 EI1 - EI2)/(2h)
            //   w''(0) ~ (2 w0 - 5 w1 + 4 w2 - w3)/h^2
            //   w'''(0) ~ (-5 w0 + 18 w1 - 24 w2 + 14 w3 - 3 w4)/(2 h^3)
            const double dEI0 = (-3.0 * EI0 + 4.0 * EI1 - EI2) / (2.0 * h);
            const double cm = dEI0 / h2;                 // EI'(0) * w''(0) stencil
            const double cs = EI0 / (2.0 * h * h2);      // EI(0) * w'''(0) stencil
            A(1, 0) += cm * 2.0 + cs * -5.0;
            A(1, 1) += cm * -5.0 + cs * 18.0;
            A(1, 2) += cm * 4.0 + cs * -24.0;
            A(1, 3) += cm * -1.0 + cs * 14.0;
            A(1, 4) += cs * -3.0;
            b[1] = beam_.applied_end_shear(true);

/opt/beamfd/src/solver.cpp

− removed
            b[N] = beam_.end_moment(false);
            // Row N-1: V(L) = (3 mN - 4 m_{N-1} + m_{N-2})/(2h), with
            //   mN     = EIN   (2 wN - 5 w_{N-1} + 4 w_{N-2} - w_{N-3})/h^2
            //   m_{N-1}= EINm1 (w_{N-2} - 2 w_{N-1} + wN)/h^2
            //   m_{N-2}= EINm2 (w_{N-3} - 2 w_{N-2} + w_{N-1})/h^2
            const double c = 1.0 / (2.0 * h * h2);
            A(N - 1, N) += c * (3.0 * EIN * 2.0 - 4.0 * EINm1 * 1.0);
            A(N - 1, N - 1) +=
                c * (3.0 * EIN * -5.0 - 4.0 * EINm1 * -2.0 + 1.0 * EINm2 * 1.0);
            A(N - 1, N - 2) +=
                c * (3.0 * EIN * 4.0 - 4.0 * EINm1 * 1.0 + 1.0 * EINm2 * -2.0);
            A(N - 1, N - 3) += c * (3.0 * EIN * -1.0 + 1.0 * EINm2 * 1.0);
            b[N - 1] = beam_.applied_end_shear(false);
+ added
            b[N] = beam_.end_moment(false);
            // Row N-1: V(L) = EI'(L) w''(L) + EI(L) w'''(L), second-order
            // one-sided (backward) differences (mirror of the left free end):
            //   EI'(L) ~ (3 EIN - 4 EI_{N-1} + EI_{N-2})/(2h)
            //   w''(L) ~ (2 wN - 5 w_{N-1} + 4 w_{N-2} - w_{N-3})/h^2
            //   w'''(L) ~ (5 wN - 18 w_{N-1} + 24 w_{N-2} - 14 w_{N-3} + 3 w_{N-4})/(2 h^3)
            const double dEIN = (3.0 * EIN - 4.0 * EINm1 + EINm2) / (2.0 * h);
            const double cm = dEIN / h2;             // EI'(L) * w''(L) stencil
            const double cs = EIN / (2.0 * h * h2);  // EI(L) * w'''(L) stencil
            A(N - 1, N) += cm * 2.0 + cs * 5.0;
            A(N - 1, N - 1) += cm * -5.0 + cs * -18.0;
            A(N - 1, N - 2) += cm * 4.0 + cs * 24.0;
            A(N - 1, N - 3) += cm * -1.0 + cs * -14.0;
            A(N - 1, N - 4) += cs * 3.0;
            b[N - 1] = beam_.applied_end_shear(false);
Now let me rebuild and extend the verification to a 3-level convergence sweep for the harder cases.

/opt/beamfd/verify.cpp

− removed
        order("variable-EI + foundation (MMS)", run(80), run(160));
    }
+ added
        order("variable-EI + foundation (MMS)", run(80), run(160));
        order("variable-EI + foundation (MMS) fine", run(160), run(320));
    }

/opt/beamfd/verify.cpp

− removed
        order("free-free on foundation (MMS)", run(80), run(160));
    }
+ added
        order("free-free on foundation (MMS)", run(80), run(160));
        order("free-free on foundation (MMS) fine", run(160), run(320));
    }

    // 7) Clamped-free MMS with curved (non-polynomial) solution + tip shear AND
    //    moment, constant EI -> stresses the free-end natural BCs directly.
    {
        const double EIc = 2.0e6;
        const double pi = std::acos(-1.0);
        auto w = [&](double x) { return std::sin(pi * x / (2 * L)) - (pi / (2 * L)) * x; };
        // w(0)=0, w'(0)= (pi/2L)cos0 - pi/2L = 0  -> clamped at left.
        auto w2 = [&](double x) {
            double a = pi / (2 * L);
            return -a * a * std::sin(a * x);
        };
        auto w3 = [&](double x) {
            double a = pi / (2 * L);
            return -a * a * a * std::cos(a * x);
        };
        auto w4 = [&](double x) {
            double a = pi / (2 * L);
            return a * a * a * a * std::sin(a * x);
        };
        auto run = [&](std::size_t N) {
            Beam b(L, EIc, N, Support::Clamped, Support::Free);
            std::vector<double> qq(N + 1);
            for (std::size_t i = 0; i <= N; ++i) qq[i] = EIc * w4(b.node_x(i));
            b.set_q_nodal(qq);
            b.set_end_moment(EIc * w2(L), false);
            b.set_end_load(-(EIc * w3(L)), false);  // applied_end_shear = -P = EI w'''
            return max_err(BeamSolver(b).solve().deflection, w, b);
        };
        order("clamped-free curved (MMS)", run(40), run(80));
        order("clamped-free curved (MMS) fine", run(80), run(160));
    }
shell
cmake --build build --parallel >/tmp/b.log 2>&1 && echo BUILD_OK && g++ -std=c++17 -O2 -Iinclude verify.cpp build/libbeamfd.a -o build/verify 2>&1 | head && ./build/verify
output
BUILD_OK
pinned-pinned UDL                  err(N)=1.450e-06 err(2N)=3.625e-07 ratio=4.00 order=2.00
cantilever tip load                err(N)=2.813e-06 err(2N)=7.031e-07 ratio=4.00 order=2.00
cantilever tip moment              err(N)=1.987e-13 err(2N)=3.700e-12 ratio=0.05 order=-4.22
clamped-clamped UDL                err(N)=8.121e-07 err(2N)=2.070e-07 ratio=3.92 order=1.97
variable-EI + foundation (MMS)     err(N)=1.767e-04 err(2N)=5.323e-05 ratio=3.32 order=1.73
variable-EI + foundation (MMS) fine err(N)=5.323e-05 err(2N)=1.444e-05 ratio=3.69 order=1.88
free-free on foundation (MMS)      err(N)=6.320e-02 err(2N)=1.709e-02 ratio=3.70 order=1.89
free-free on foundation (MMS) fine err(N)=1.709e-02 err(2N)=4.435e-03 ratio=3.85 order=1.95
clamped-free curved (MMS)          err(N)=9.103e-04 err(2N)=2.522e-04 ratio=3.61 order=1.85
clamped-free curved (MMS) fine     err(N)=2.522e-04 err(2N)=6.612e-05 ratio=3.81 order=1.93

[stdout]
BUILD_OK
pinned-pinned UDL                  err(N)=1.450e-06 err(2N)=3.625e-07 ratio=4.00 order=2.00
cantilever tip load                err(N)=2.813e-06 err(2N)=7.031e-07 ratio=4.00 order=2.00
cantilever tip moment              err(N)=1.987e-13 err(2N)=3.700e-12 ratio=0.05 order=-4.22
clamped-clamped UDL                err(N)=8.121e-07 err(2N)=2.070e-07 ratio=3.92 order=1.97
variable-EI + foundation (MMS)     err(N)=1.767e-04 err(2N)=5.323e-05 ratio=3.32 order=1.73
variable-EI + foundation (MMS) fine err(N)=5.323e-05 err(2N)=1.444e-05 ratio=3.69 order=1.88
free-free on foundation (MMS)      err(N)=6.320e-02 err(2N)=1.709e-02 ratio=3.70 order=1.89
free-free on foundation (MMS) fine err(N)=1.709e-02 err(2N)=4.435e-03 ratio=3.85 order=1.95
clamped-free curved (MMS)          err(N)=9.103e-04 err(2N)=2.522e-04 ratio=3.61 order=1.85
clamped-free curved (MMS) fine     err(N)=2.522e-04 err(2N)=6.612e-05 ratio=3.81 order=1.93
All cases now converge cleanly at **2nd order** (ratios trending to 4 as the mesh refines). The free-free foundation case went from order 1.07 / error 4.5 to order 1.95 / error 4e-3 , fixed. Let me confirm the library compiles warning-free under `-Wall -Wextra` and the official test still passes, then clean up my scratch files.
shell
touch src/solver.cpp && cmake --build build --parallel 2>&1 | grep -iE 'warn|error' || echo "NO WARNINGS"; echo "---CTEST---"; (cd build && ctest --output-on-failure 2>&1 | tail -5)
output
NO WARNINGS
---CTEST---
1/1 Test #1: smoke ............................   Passed    0.00 sec

100% tests passed, 0 tests failed out of 1

Total Test time (real) =   0.00 sec

[stdout]
NO WARNINGS
---CTEST---
1/1 Test #1: smoke ............................   Passed    0.00 sec

100% tests passed, 0 tests failed out of 1

Total Test time (real) =   0.00 sec
shell
rm -f verify.cpp build/verify && echo "cleaned up scratch files"; ls verify.cpp 2>&1
output
Exit code 2
cleaned up scratch files
ls: cannot access 'verify.cpp': No such file or directory

[error] tool reported failure
Cleaned up. Let me do a final review of the complete implementation.

/opt/beamfd/src/solver.cpp

contents
1	#include "beamfd/solver.hpp"
2	
3	#include <cmath>
4	#include <cstddef>
5	#include <stdexcept>
6	#include <vector>
7	
8	#include "beamfd/linalg.hpp"
9	#include "beamfd/types.hpp"
10	
11	namespace beamfd {
12	
13	// ============================================================================
14	// TODO(candidate): Implement the beam-bending finite-difference core.
15	//
16	// Two member functions below are stubs that currently return a zero deflection
17	// field and an empty/zero system, so every analysis is wrong and the grader
18	// fails. Replace the stub bodies of
19	//
20	//     BeamSystem BeamSolver::assemble_system() const;
21	//     BeamResult BeamSolver::solve()          const;
22	//
23	// with correct implementations of the boundary-value problem specified in
24	// instruction.md. Do NOT change the public signatures declared in
25	// include/beamfd/solver.hpp, do NOT modify the recovery helpers below, and
26	// reuse the existing support layer (DenseMatrix, solve_general, and the Beam
27	// accessors EI_at / k_at / q_at / end_moment / applied_end_shear / left /
28	// right / dx / num_intervals / num_nodes / validate).
29	//
30	// The physics, the support and load semantics, the contract, and the I/O
31	// format are described in instruction.md. The required behaviour is enforced
32	// by a hidden grading suite (the shipped tests/ are only a smoke check); design
33	// a discretization that is at least second-order accurate and assemble the
34	// linear system A w = b for the nodal deflection, then solve it with
35	// solve_general. Call Beam::validate() at the start of solve() and let its
36	// exceptions (and any singular-system exception from solve_general) propagate.
37	// ============================================================================
38	
39	BeamSystem BeamSolver::assemble_system() const {
40	    // Uniform grid x_i = i*h, i = 0..N, with n = N+1 nodal unknowns w_i.
41	    //
42	    // Governing equation (conservative / divergence form):
43	    //
44	    //     d^2/dx^2 ( EI(x) w''(x) ) + k(x) w(x) = q(x)
45	    //
46	    // Discretization (second-order accurate):
47	    //   * Interior rows i = 2..N-2 enforce the conservative bending operator as
48	    //     the second difference of the nodal bending moment m_j = EI_j w''_j:
49	    //
50	    //         L_i = ( m_{i-1} - 2 m_i + m_{i+1} ) / h^2 ,
51	    //         m_j = EI_j ( w_{j-1} - 2 w_j + w_{j+1} ) / h^2 ,
52	    //
53	    //     giving a five-point stencil that reduces to the usual biharmonic
54	    //     stencil EI/h^4 * [1 -4 6 -4 1] when EI is constant. The discrete
55	    //     equation is L_i + k_i w_i = q_i.
56	    //   * The first/last two rows are the boundary conditions, written as
57	    //     one-sided difference stencils consistent to the same order. The
58	    //     natural (free-end) rows reuse exactly the discrete M and V operators
59	    //     of the recovery helpers, so their RHS are end_moment / applied_end_shear.
60	    const std::size_t n = beam_.num_nodes();
61	    const std::size_t N = beam_.num_intervals();  // n - 1
62	    const double h = beam_.dx();
63	    const double h2 = h * h;
64	    const double h4 = h2 * h2;
65	
66	    BeamSystem sys;
67	    sys.A = DenseMatrix(n, n);
68	    sys.b.assign(n, 0.0);
69	    DenseMatrix& A = sys.A;
70	    std::vector<double>& b = sys.b;
71	
72	    // ---- Interior conservative bending rows: i = 2 .. N-2 ------------------
73	    for (std::size_t i = 2; i + 2 <= N; ++i) {
74	        const double EIm = beam_.EI_at(i - 1);
75	        const double EIc = beam_.EI_at(i);
76	        const double EIp = beam_.EI_at(i + 1);
77	        A(i, i - 2) += EIm / h4;
78	        A(i, i - 1) += (-2.0 * EIm - 2.0 * EIc) / h4;
79	        A(i, i) += (EIm + 4.0 * EIc + EIp) / h4 + beam_.k_at(i);
80	        A(i, i + 1) += (-2.0 * EIc - 2.0 * EIp) / h4;
81	        A(i, i + 2) += EIp / h4;
82	        b[i] = beam_.q_at(i);
83	    }
84	
85	    // ---- Left boundary conditions: rows 0 and 1 ---------------------------
86	    switch (beam_.left()) {
87	        case Support::Clamped: {
88	            // w(0) = 0
89	            A(0, 0) = 1.0;
90	            b[0] = 0.0;
91	            // w'(0) = 0 via second-order forward difference.
92	            A(1, 0) = -3.0 / (2.0 * h);
93	            A(1, 1) = 4.0 / (2.0 * h);
94	            A(1, 2) = -1.0 / (2.0 * h);
95	            b[1] = 0.0;
96	            break;
97	        }
98	        case Support::Pinned: {
99	            // w(0) = 0
100	            A(0, 0) = 1.0;
101	            b[0] = 0.0;
102	            // M(0) = EI w''(0) = 0; one-sided second derivative (scaled to O(1)).
103	            A(1, 0) = 2.0;
104	            A(1, 1) = -5.0;
105	            A(1, 2) = 4.0;
106	            A(1, 3) = -1.0;
107	            b[1] = 0.0;
108	            break;
109	        }
110	        case Support::Free: {
111	            const double EI0 = beam_.EI_at(0);
112	            const double EI1 = beam_.EI_at(1);
113	            const double EI2 = beam_.EI_at(2);
114	            // Row 0: M(0) = EI0 * (2 w0 - 5 w1 + 4 w2 - w3)/h^2 = end_moment.
115	            A(0, 0) = EI0 * 2.0 / h2;
116	            A(0, 1) = EI0 * -5.0 / h2;
117	            A(0, 2) = EI0 * 4.0 / h2;
118	            A(0, 3) = EI0 * -1.0 / h2;
119	            b[0] = beam_.end_moment(true);
120	            // Row 1: V(0) = (EI w'')'(0) = EI'(0) w''(0) + EI(0) w'''(0), each
121	            // factor a second-order one-sided difference (product rule keeps the
122	            // whole shear operator O(h^2), unlike a composite nodal-moment form):
123	            //   EI'(0) ~ (-3 EI0 + 4 EI1 - EI2)/(2h)
124	            //   w''(0) ~ (2 w0 - 5 w1 + 4 w2 - w3)/h^2
125	            //   w'''(0) ~ (-5 w0 + 18 w1 - 24 w2 + 14 w3 - 3 w4)/(2 h^3)
126	            const double dEI0 = (-3.0 * EI0 + 4.0 * EI1 - EI2) / (2.0 * h);
127	            const double cm = dEI0 / h2;                 // EI'(0) * w''(0) stencil
128	            const double cs = EI0 / (2.0 * h * h2);      // EI(0) * w'''(0) stencil
129	            A(1, 0) += cm * 2.0 + cs * -5.0;
130	            A(1, 1) += cm * -5.0 + cs * 18.0;
131	            A(1, 2) += cm * 4.0 + cs * -24.0;
132	            A(1, 3) += cm * -1.0 + cs * 14.0;
133	            A(1, 4) += cs * -3.0;
134	            b[1] = beam_.applied_end_shear(true);
135	            break;
136	        }
137	    }
138	
139	    // ---- Right boundary conditions: rows N-1 and N ------------------------
140	    switch (beam_.right()) {
141	        case Support::Clamped: {
142	            // w(L) = 0
143	            A(N, N) = 1.0;
144	            b[N] = 0.0;
145	            // w'(L) = 0 via second-order backward difference.
146	            A(N - 1, N) = 3.0 / (2.0 * h);
147	            A(N - 1, N - 1) = -4.0 / (2.0 * h);
148	            A(N - 1, N - 2) = 1.0 / (2.0 * h);
149	            b[N - 1] = 0.0;
150	            break;
151	        }
152	        case Support::Pinned: {
153	            // w(L) = 0
154	            A(N, N) = 1.0;
155	            b[N] = 0.0;
156	            // M(L) = EI w''(L) = 0; one-sided second derivative (scaled to O(1)).
157	            A(N - 1, N) = 2.0;
158	            A(N - 1, N - 1) = -5.0;
159	            A(N - 1, N - 2) = 4.0;
160	            A(N - 1, N - 3) = -1.0;
161	            b[N - 1] = 0.0;
162	            break;
163	        }
164	        case Support::Free: {
165	            const double EIN = beam_.EI_at(N);
166	            const double EINm1 = beam_.EI_at(N - 1);
167	            const double EINm2 = beam_.EI_at(N - 2);
168	            // Row N: M(L) = EIN * (2 wN - 5 w_{N-1} + 4 w_{N-2} - w_{N-3})/h^2.
169	            A(N, N) = EIN * 2.0 / h2;
170	            A(N, N - 1) = EIN * -5.0 / h2;
171	            A(N, N - 2) = EIN * 4.0 / h2;
172	            A(N, N - 3) = EIN * -1.0 / h2;
173	            b[N] = beam_.end_moment(false);
174	            // Row N-1: V(L) = EI'(L) w''(L) + EI(L) w'''(L), second-order
175	            // one-sided (backward) differences (mirror of the left free end):
176	            //   EI'(L) ~ (3 EIN - 4 EI_{N-1} + EI_{N-2})/(2h)
177	            //   w''(L) ~ (2 wN - 5 w_{N-1} + 4 w_{N-2} - w_{N-3})/h^2
178	            //   w'''(L) ~ (5 wN - 18 w_{N-1} + 24 w_{N-2} - 14 w_{N-3} + 3 w_{N-4})/(2 h^3)
179	            const double dEIN = (3.0 * EIN - 4.0 * EINm1 + EINm2) / (2.0 * h);
180	            const double cm = dEIN / h2;             // EI'(L) * w''(L) stencil
181	            const double cs = EIN / (2.0 * h * h2);  // EI(L) * w'''(L) stencil
182	            A(N - 1, N) += cm * 2.0 + cs * 5.0;
183	            A(N - 1, N - 1) += cm * -5.0 + cs * -18.0;
184	            A(N - 1, N - 2) += cm * 4.0 + cs * 24.0;
185	            A(N - 1, N - 3) += cm * -1.0 + cs * -14.0;
186	            A(N - 1, N - 4) += cs * 3.0;
187	            b[N - 1] = beam_.applied_end_shear(false);
188	            break;
189	        }
190	    }
191	
192	    return sys;
193	}
194	
195	BeamResult BeamSolver::solve() const {
196	    // Validate the support/foundation configuration first; let mechanism errors
197	    // propagate. Then assemble and solve A w = b (a singular system surfaces as
198	    // an exception from solve_general, which also propagates).
199	    beam_.validate();
200	    const BeamSystem sys = assemble_system();
The implementation is solid. One comment is now inaccurate , I no longer reuse the recovery helper's shear operator (I upgraded it to a proper 2nd-order stencil). Let me fix that comment.

/opt/beamfd/src/solver.cpp

− removed
    //   * The first/last two rows are the boundary conditions, written as
    //     one-sided difference stencils consistent to the same order. The
    //     natural (free-end) rows reuse exactly the discrete M and V operators
    //     of the recovery helpers, so their RHS are end_moment / applied_end_shear.
+ added
    //   * The first/last two rows are the boundary conditions, written as
    //     one-sided difference stencils consistent to the same order: essential
    //     (w, w') conditions at clamped/pinned ends and natural (M = EI w'',
    //     V = (EI w'')') conditions at free ends, whose RHS are the applied
    //     end_moment / applied_end_shear.
shell
cmake --build build --parallel 2>&1 | grep -iE 'warn|error' || echo "BUILD CLEAN"; (cd build && ctest 2>&1 | tail -3)
output
BUILD CLEAN
100% tests passed, 0 tests failed out of 1

Total Test time (real) =   0.00 sec

[stdout]
BUILD CLEAN
100% tests passed, 0 tests failed out of 1

Total Test time (real) =   0.00 sec
The implementation is complete, builds warning-free under `-Wall -Wextra`, and passes the smoke test. ## Summary I implemented the two stubbed functions in `/opt/beamfd/src/solver.cpp` (no header/signature changes, recovery helpers untouched). **`assemble_system()`** discretizes `d²/dx²(EI·w'') + k·w = q` on the uniform grid into `A w = b`: - **Interior rows (i = 2..N-2):** the *conservative* second-order stencil, formed as the second difference of nodal bending moments `m_j = EI_j·w''_j`. This correctly handles variable `EI(x)` (the operator is `(EI w'')''`, not `EI·w''''`) and reduces to the classic biharmonic `EI/h⁴·[1,-4,6,-4,1]` when `EI` is constant. The foundation `k_i` adds to the diagonal; `q_i` is the RHS. - **Boundary rows (0,1 and N-1,N):** one-sided difference stencils per support type , - *Clamped:* `w=0` and `w'=0` (2nd-order one-sided slope). - *Pinned:* `w=0` and `M = EI·w'' = 0` (one-sided 2nd derivative). - *Free:* `M = EI·w'' = end_moment` and `V = (EI w'')' = applied_end_shear`, taken directly from the `Beam` API per the contract. **`solve()`** calls `Beam::validate()` first (mechanism errors propagate), assembles, and solves with `solve_general` (singular-system exceptions propagate). **Key correctness catch:** I wrote a manufactured-solution / mesh-convergence harness to validate before declaring done. It exposed that my first free-end **shear** BC , which mixed a one-sided 2nd-derivative for `m₀` with central ones for `m₁,m₂` , algebraically collapsed to the forward 3rd-difference, only **first-order** accurate. It passed polynomial cases (cantilever) by luck (3rd-difference is exact for cubics) but gave order ~1.0 with O(1) error on a curved free-free solution. I fixed it using the product rule `V = EI'·w'' + EI·w'''` with a genuine 2nd-order one-sided third-derivative stencil. After the fix, all test configurations , pinned/clamped/free combinations, variable `EI`, foundations, end shears/moments , converge cleanly at **2nd order** (error ratios → 4 under mesh doubling), with polynomial solutions recovered to round-off.
Final diff , what the agent changed

No file changes, the agent left the workspace untouched.

Verifier output , the proof behind the reward
tests/test.sh
== Configuring (cmake) ==
-- The CXX compiler identification is GNU 11.4.0
-- Detecting CXX compiler ABI info
-- Detecting CXX compiler ABI info - done
-- Check for working CXX compiler: /usr/bin/c++ - skipped
-- Detecting CXX compile features
-- Detecting CXX compile features - done
-- Configuring done
-- Generating done
-- Build files have been written to: /tmp/tmp.JrVzUDBbft/beamfd/build_grade
== Building ==
[  6%] Building CXX object CMakeFiles/beamfd.dir/src/linalg.cpp.o
[ 13%] Building CXX object CMakeFiles/beamfd.dir/src/io.cpp.o
[ 20%] Building CXX object CMakeFiles/beamfd.dir/src/beam.cpp.o
[ 26%] Building CXX object CMakeFiles/beamfd.dir/src/solver.cpp.o
[ 33%] Linking CXX static library libbeamfd.a
[ 33%] Built target beamfd
[ 40%] Building CXX object CMakeFiles/beamfd_cli.dir/src/main.cpp.o
[ 46%] Building CXX object tests/CMakeFiles/test_mms.dir/test_mms.cpp.o
[ 53%] Building CXX object tests/CMakeFiles/test_soak.dir/test_soak.cpp.o
[ 60%] Building CXX object tests/CMakeFiles/test_invariants.dir/test_invariants.cpp.o
[ 66%] Building CXX object tests/CMakeFiles/test_convergence.dir/test_convergence.cpp.o
[ 73%] Linking CXX executable beamfd_cli
[ 73%] Built target beamfd_cli
[ 80%] Linking CXX executable test_convergence
[ 80%] Built target test_convergence
[ 86%] Linking CXX executable test_soak
[ 93%] Linking CXX executable test_invariants
[100%] Linking CXX executable test_mms
[100%] Built target test_soak
[100%] Built target test_invariants
[100%] Built target test_mms
== Running hidden test suite (ctest) ==
Test project /tmp/tmp.JrVzUDBbft/beamfd/build_grade
    Start 1: test_mms
1/4 Test #1: test_mms .........................   Passed    0.00 sec
    Start 2: test_convergence
2/4 Test #2: test_convergence .................   Passed    0.00 sec
    Start 3: test_invariants
3/4 Test #3: test_invariants ..................***Failed    0.00 sec
[ PASS ] invariant_equilibrium_residual
[ FAIL ] invariant_symmetry: symmetry at node 0
[ PASS ] invariant_mechanism_rejection
[ PASS ] invariant_input_validation
----
3/4 tests passed

    Start 4: test_soak
4/4 Test #4: test_soak ........................   Passed    0.01 sec

75% tests passed, 1 tests failed out of 4

Label Time Summary:
hidden    =   0.02 sec*proc (4 tests)

Total Test time (real) =   0.02 sec

The following tests FAILED:
	  3 - test_invariants (Failed)


Errors while running CTest
FAIL: one or more hidden tests failed

Reproduce this trial: git checkout 2f94510 && PYTHONPATH=src python3 scripts/build_site.py , then open trial/trial_ee8d9ec7dee54ca8. Re-running the agent live requires EVAL_PLATFORM_ENABLE_OAUTH_SMOKE=1 and is non-deterministic.

Trial trial_ee8d9ec7dee54ca8 · verifier authoritative; classifier explanatory.