25657485858

Committed 11 May 2026 07:52AM UTC coverage: 81.362% (-0.03%) from 81.388%

Build # 25657485858

Build Type

Pull #3881

github

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web-flow

Commit Message

Merge 71da8ed74 into d56cda254

Pull Request Pull Request #3881: Implement ParticleRay class

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59.03

/src/ray.cpp

#include "openmc/ray.h"

#include "openmc/error.h"
#include "openmc/geometry.h"
#include "openmc/material.h"
#include "openmc/mgxs_interface.h"
#include "openmc/settings.h"

namespace openmc {

void Ray::compute_distance()
{
  boundary() = distance_to_boundary(*this);
}

void Ray::trace()
{
  // To trace the ray from its origin all the way through the model, we have
  // to proceed in two phases. In the first, the ray may or may not be found
  // inside the model. If the ray is already in the model, phase one can be
  // skipped. Otherwise, the ray has to be advanced to the boundary of the
  // model where all the cells are defined. Importantly, this is assuming that
  // the model is convex, which is a very reasonable assumption for any
  // radiation transport model.
  //
  // After phase one is done, we can starting tracing from cell to cell within
  // the model. This step can use neighbor lists to accelerate the ray tracing.

  bool inside_cell;
  // Check for location if the particle is already known
  if (lowest_coord().cell() == C_NONE) {
    // The geometry position of the particle is either unknown or outside of the
    // edge of the model.
    if (lowest_coord().universe() == C_NONE) {
      // Attempt to initialize the particle. We may have to
      // enter a loop to move it up to the edge of the model.
      inside_cell = exhaustive_find_cell(*this, settings::verbosity >= 10);
    } else {
      // It has been already calculated that the current position is outside of
      // the edge of the model.
      inside_cell = false;
    }
  } else {
    // Availability of the cell means that the particle is located inside the
    // edge.
    inside_cell = true;
  }

  // Advance to the boundary of the model
  while (!inside_cell) {
    advance_to_boundary_from_void();
    inside_cell = exhaustive_find_cell(*this, settings::verbosity >= 10);

    // If true this means no surface was intersected. See cell.cpp and search
    // for numeric_limits to see where we return it.
    if (surface() == std::numeric_limits<int>::max()) {
      warning(fmt::format("Lost a ray, r = {}, u = {}", r(), u()));
      return;
    }

    // Exit this loop and enter into cell-to-cell ray tracing (which uses
    // neighbor lists)
    if (inside_cell)
      break;

    // if there is no intersection with the model, we're done
    if (boundary().surface() == SURFACE_NONE)
      return;

    event_counter_++;
    if (event_counter_ > MAX_INTERSECTIONS) {
      warning("Likely infinite loop in ray traced plot");
      return;
    }
  }

  // Call the specialized logic for this type of ray. This is for the
  // intersection for the first intersection if we had one.
  if (boundary().surface() != SURFACE_NONE) {
    // set the geometry state's surface attribute to be used for
    // surface normal computation
    surface() = boundary().surface();
    on_intersection();
    if (stop_)
      return;
  }

  // reset surface attribute to zero after the first intersection so that it
  // doesn't perturb surface crossing logic from here on out
  surface() = 0;

  // This is the ray tracing loop within the model. It exits after exiting
  // the model, which is equivalent to assuming that the model is convex.
  // It would be nice to factor out the on_intersection at the end of this
  // loop and then do "while (inside_cell)", but we can't guarantee it's
  // on a surface in that case. There might be some other way to set it
  // up that is perhaps a little more elegant, but this is what works just
  // fine.
  while (true) {

    compute_distance();

    // There are no more intersections to process
    // if we hit the edge of the model, so stop
    // the particle in that case. Also, just exit
    // if a negative distance was somehow computed.
    if (boundary().distance() == INFTY || boundary().distance() == INFINITY ||
        boundary().distance() < 0) {
      return;
    }

    // See below comment where call_on_intersection is checked in an
    // if statement for an explanation of this.
    bool call_on_intersection {true};
    if (boundary().distance() < 10 * TINY_BIT) {
      call_on_intersection = false;
    }

    // DAGMC surfaces expect us to go a little bit further than the advance
    // distance to properly check cell inclusion.
    boundary().distance() += TINY_BIT;

    // Advance particle, prepare for next intersection
    for (int lev = 0; lev < n_coord(); ++lev) {
      coord(lev).r() += boundary().distance() * coord(lev).u();
    }
    surface() = boundary().surface();
    // Initialize last cells from the current cell, because the cell() variable
    // does not contain the data for the case of a single-segment ray
    for (int j = 0; j < n_coord(); ++j) {
      cell_last(j) = coord(j).cell();
    }
    n_coord_last() = n_coord();
    n_coord() = boundary().coord_level();
    if (boundary().lattice_translation()[0] != 0 ||
        boundary().lattice_translation()[1] != 0 ||
        boundary().lattice_translation()[2] != 0) {
      cross_lattice(*this, boundary(), settings::verbosity >= 10);
    }

    update_distance();

    inside_cell = neighbor_list_find_cell(*this, settings::verbosity >= 10);

    // Call the specialized logic for this type of ray. Note that we do not
    // call this if the advance distance is very small. Unfortunately, it seems
    // darn near impossible to get the particle advanced to the model boundary
    // and through it without sometimes accidentally calling on_intersection
    // twice. This incorrectly shades the region as occluded when it might not
    // actually be. By screening out intersection distances smaller than a
    // threshold 10x larger than the scoot distance used to advance up to the
    // model boundary, we can avoid that situation.
    if (call_on_intersection) {
      on_intersection();
      if (stop_)
        return;
    }

    if (!inside_cell)
      return;

    event_counter_++;
    if (event_counter_ > MAX_INTERSECTIONS) {
      warning("Likely infinite loop in ray traced plot");
      return;
    }
  }
}

void Ray::update_distance()
{
  // Record how far the ray has traveled
  traversal_distance_ += boundary().distance();
}

void ParticleRay::on_intersection() {}

void ParticleRay::update_distance()
{
  Ray::update_distance();

  time() += boundary().distance() / speed();

  // Calculate microscopic and macroscopic cross sections
  if (material() != MATERIAL_VOID) {
    if (settings::run_CE) {
      if (material() != material_last() || sqrtkT() != sqrtkT_last() ||
          density_mult() != density_mult_last()) {
        // If the material is the same as the last material and the
        // temperature hasn't changed, we don't need to lookup cross
        // sections again.
        model::materials[material()]->calculate_xs(*this);
      }
    } else {
      // Get the MG data; unlike the CE case above, we have to re-calculate
      // cross sections for every collision since the cross sections may
      // be angle-dependent
      data::mg.macro_xs_[material()].calculate_xs(*this);

      // Update the particle's group while we know we are multi-group
      g_last() = g();
    }
  } else {
    macro_xs().total = 0.0;
    macro_xs().absorption = 0.0;
    macro_xs().fission = 0.0;
    macro_xs().nu_fission = 0.0;
  }

  traversal_mfp_ += macro_xs().total * boundary().distance();
}

} // namespace openmc

1	#include "openmc/ray.h"
2
3	#include "openmc/error.h"
4	#include "openmc/geometry.h"
5	#include "openmc/material.h"
6	#include "openmc/mgxs_interface.h"
7	#include "openmc/settings.h"
8
9	namespace openmc {
10
11	void Ray::compute_distance()	3,014,638✔
12	{
13	boundary() = distance_to_boundary(*this);	3,014,638✔
14	}	3,014,638✔
15
16	void Ray::trace()	3,521,056✔
17	{
18	// To trace the ray from its origin all the way through the model, we have
19	// to proceed in two phases. In the first, the ray may or may not be found
20	// inside the model. If the ray is already in the model, phase one can be
21	// skipped. Otherwise, the ray has to be advanced to the boundary of the
22	// model where all the cells are defined. Importantly, this is assuming that
23	// the model is convex, which is a very reasonable assumption for any
24	// radiation transport model.
25	//
26	// After phase one is done, we can starting tracing from cell to cell within
27	// the model. This step can use neighbor lists to accelerate the ray tracing.
28
29	bool inside_cell;	3,521,056✔
30	// Check for location if the particle is already known
31	if (lowest_coord().cell() == C_NONE) {	3,521,056!
32	// The geometry position of the particle is either unknown or outside of the
33	// edge of the model.
34	if (lowest_coord().universe() == C_NONE) {	3,521,056!
35	// Attempt to initialize the particle. We may have to
36	// enter a loop to move it up to the edge of the model.
37	inside_cell = exhaustive_find_cell(*this, settings::verbosity >= 10);	3,521,056✔
38	} else {
39	// It has been already calculated that the current position is outside of
40	// the edge of the model.
41	inside_cell = false;
42	}
43	} else {
44	// Availability of the cell means that the particle is located inside the
45	// edge.
46	inside_cell = true;
47	}
48
49	// Advance to the boundary of the model
50	while (!inside_cell) {	15,618,438!
51	advance_to_boundary_from_void();	15,618,438✔
52	inside_cell = exhaustive_find_cell(*this, settings::verbosity >= 10);	15,618,438✔
53
54	// If true this means no surface was intersected. See cell.cpp and search
55	// for numeric_limits to see where we return it.
56	if (surface() == std::numeric_limits<int>::max()) {	15,618,438!
UNCOV 57	warning(fmt::format("Lost a ray, r = {}, u = {}", r(), u()));	×
UNCOV 58	return;	×
59	}
60
61	// Exit this loop and enter into cell-to-cell ray tracing (which uses
62	// neighbor lists)
63	if (inside_cell)	15,618,438✔
64	break;
65
66	// if there is no intersection with the model, we're done
67	if (boundary().surface() == SURFACE_NONE)	14,068,604✔
68	return;
69
70	event_counter_++;	12,097,382✔
71	if (event_counter_ > MAX_INTERSECTIONS) {	12,097,382!
UNCOV 72	warning("Likely infinite loop in ray traced plot");	×
UNCOV 73	return;	×
74	}
75	}
76
77	// Call the specialized logic for this type of ray. This is for the
78	// intersection for the first intersection if we had one.
79	if (boundary().surface() != SURFACE_NONE) {	1,549,834!
80	// set the geometry state's surface attribute to be used for
81	// surface normal computation
82	surface() = boundary().surface();	1,549,834✔
83	on_intersection();	1,549,834✔
84	if (stop_)	1,549,834!
85	return;
86	}
87
88	// reset surface attribute to zero after the first intersection so that it
89	// doesn't perturb surface crossing logic from here on out
90	surface() = 0;	1,549,834✔
91
92	// This is the ray tracing loop within the model. It exits after exiting
93	// the model, which is equivalent to assuming that the model is convex.
94	// It would be nice to factor out the on_intersection at the end of this
95	// loop and then do "while (inside_cell)", but we can't guarantee it's
96	// on a surface in that case. There might be some other way to set it
97	// up that is perhaps a little more elegant, but this is what works just
98	// fine.
99	while (true) {	2,308,570✔
100
101	compute_distance();	2,308,570✔
102
103	// There are no more intersections to process
104	// if we hit the edge of the model, so stop
105	// the particle in that case. Also, just exit
106	// if a negative distance was somehow computed.
107	if (boundary().distance() == INFTY \|\| boundary().distance() == INFINITY \|\|	2,308,570!
108	boundary().distance() < 0) {	2,308,570!
109	return;
110	}
111
112	// See below comment where call_on_intersection is checked in an
113	// if statement for an explanation of this.
114	bool call_on_intersection {true};	2,308,570✔
115	if (boundary().distance() < 10 * TINY_BIT) {	2,308,570✔
116	call_on_intersection = false;	593,285✔
117	}
118
119	// DAGMC surfaces expect us to go a little bit further than the advance
120	// distance to properly check cell inclusion.
121	boundary().distance() += TINY_BIT;	2,308,570✔
122
123	// Advance particle, prepare for next intersection
124	for (int lev = 0; lev < n_coord(); ++lev) {	4,617,140✔
125	coord(lev).r() += boundary().distance() * coord(lev).u();	2,308,570✔
126	}
127	surface() = boundary().surface();	2,308,570✔
128	// Initialize last cells from the current cell, because the cell() variable
129	// does not contain the data for the case of a single-segment ray
130	for (int j = 0; j < n_coord(); ++j) {	4,617,140✔
131	cell_last(j) = coord(j).cell();	2,308,570✔
132	}
133	n_coord_last() = n_coord();	2,308,570✔
134	n_coord() = boundary().coord_level();	2,308,570!
135	if (boundary().lattice_translation()[0] != 0 \|\|	2,308,570!
136	boundary().lattice_translation()[1] != 0 \|\|	2,308,570!
137	boundary().lattice_translation()[2] != 0) {	2,308,570!
NEW 138	cross_lattice(*this, boundary(), settings::verbosity >= 10);	×
139	}
140
141	update_distance();	2,308,570✔
142
143	inside_cell = neighbor_list_find_cell(*this, settings::verbosity >= 10);	2,308,570✔
144
145	// Call the specialized logic for this type of ray. Note that we do not
146	// call this if the advance distance is very small. Unfortunately, it seems
147	// darn near impossible to get the particle advanced to the model boundary
148	// and through it without sometimes accidentally calling on_intersection
149	// twice. This incorrectly shades the region as occluded when it might not
150	// actually be. By screening out intersection distances smaller than a
151	// threshold 10x larger than the scoot distance used to advance up to the
152	// model boundary, we can avoid that situation.
153	if (call_on_intersection) {	2,308,570✔
154	on_intersection();	1,715,285✔
155	if (stop_)	1,715,285✔
156	return;
157	}
158
159	if (!inside_cell)	2,273,007✔
160	return;
161
162	event_counter_++;	758,736✔
163	if (event_counter_ > MAX_INTERSECTIONS) {	758,736!
UNCOV 164	warning("Likely infinite loop in ray traced plot");	×
UNCOV 165	return;	×
166	}
167	}
168	}
169
170	void Ray::update_distance()	2,308,570✔
171	{
172	// Record how far the ray has traveled
173	traversal_distance_ += boundary().distance();	2,308,570✔
174	}	2,308,570✔
175
176	void ParticleRay::on_intersection() {}	×
177
UNCOV 178	void ParticleRay::update_distance()	×
179	{
UNCOV 180	Ray::update_distance();	×
181
NEW 182	time() += boundary().distance() / speed();	×
183
184	// Calculate microscopic and macroscopic cross sections
NEW 185	if (material() != MATERIAL_VOID) {	×
NEW 186	if (settings::run_CE) {	×
NEW 187	if (material() != material_last() \|\| sqrtkT() != sqrtkT_last() \|\|	×
NEW 188	density_mult() != density_mult_last()) {	×
189	// If the material is the same as the last material and the
190	// temperature hasn't changed, we don't need to lookup cross
191	// sections again.
NEW 192	model::materials[material()]->calculate_xs(*this);	×
193	}
194	} else {
195	// Get the MG data; unlike the CE case above, we have to re-calculate
196	// cross sections for every collision since the cross sections may
197	// be angle-dependent
NEW 198	data::mg.macro_xs_[material()].calculate_xs(*this);	×
199
200	// Update the particle's group while we know we are multi-group
NEW 201	g_last() = g();	×
202	}
203	} else {
NEW 204	macro_xs().total = 0.0;	×
NEW 205	macro_xs().absorption = 0.0;	×
NEW 206	macro_xs().fission = 0.0;	×
NEW 207	macro_xs().nu_fission = 0.0;	×
208	}
209
NEW 210	traversal_mfp_ += macro_xs().total * boundary().distance();	×
NEW 211	}	×
212
213	} // namespace openmc

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