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SWIFT
SWIFTsim
Commits
8632501a
Commit
8632501a
authored
7 years ago
by
Matthieu Schaller
Browse files
Options
Downloads
Patches
Plain Diff
Removed the old un-vectorized version of the gravity P-P interaction.
parent
4a20260b
Branches
Branches containing commit
Tags
Tags containing commit
1 merge request
!420
Gravity speedup
Changes
1
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1 changed file
src/runner_doiact_grav.h
+2
-358
2 additions, 358 deletions
src/runner_doiact_grav.h
with
2 additions
and
358 deletions
src/runner_doiact_grav.h
+
2
−
358
View file @
8632501a
...
...
@@ -301,7 +301,7 @@ void runner_dopair_grav_pp_full(struct runner *r, struct cell *ci,
/* Now do the opposite loop */
if
(
cj_active
)
{
/* Loop over all particles in c
i
... */
/* Loop over all particles in c
j
... */
for
(
int
pjd
=
0
;
pjd
<
gcount_j
;
pjd
++
)
{
/* Skip inactive particles */
...
...
@@ -394,106 +394,6 @@ void runner_dopair_grav_pp_full(struct runner *r, struct cell *ci,
/* Write back to the particles */
if
(
ci_active
)
gravity_cache_write_back
(
ci_cache
,
gparts_i
,
gcount_i
);
if
(
cj_active
)
gravity_cache_write_back
(
cj_cache
,
gparts_j
,
gcount_j
);
#ifdef MATTHIEU_OLD_STUFF
/* Some constants */
const
struct
engine
*
const
e
=
r
->
e
;
/* Cell properties */
const
int
gcount_i
=
ci
->
gcount
;
const
int
gcount_j
=
cj
->
gcount
;
struct
gpart
*
restrict
gparts_i
=
ci
->
gparts
;
struct
gpart
*
restrict
gparts_j
=
cj
->
gparts
;
/* MATTHIEU: Should we use local DP accumulators ? */
/* Loop over all particles in ci... */
if
(
cell_is_active
(
ci
,
e
))
{
for
(
int
pid
=
0
;
pid
<
gcount_i
;
pid
++
)
{
/* Get a hold of the ith part in ci. */
struct
gpart
*
restrict
gpi
=
&
gparts_i
[
pid
];
if
(
!
gpart_is_active
(
gpi
,
e
))
continue
;
/* Apply boundary condition */
const
double
pix
[
3
]
=
{
gpi
->
x
[
0
]
-
shift
[
0
],
gpi
->
x
[
1
]
-
shift
[
1
],
gpi
->
x
[
2
]
-
shift
[
2
]};
/* Loop over every particle in the other cell. */
for
(
int
pjd
=
0
;
pjd
<
gcount_j
;
pjd
++
)
{
/* Get a hold of the jth part in cj. */
const
struct
gpart
*
restrict
gpj
=
&
gparts_j
[
pjd
];
/* Compute the pairwise distance. */
const
float
dx
[
3
]
=
{
pix
[
0
]
-
gpj
->
x
[
0
],
// x
pix
[
1
]
-
gpj
->
x
[
1
],
// y
pix
[
2
]
-
gpj
->
x
[
2
]};
// z
const
float
r2
=
dx
[
0
]
*
dx
[
0
]
+
dx
[
1
]
*
dx
[
1
]
+
dx
[
2
]
*
dx
[
2
];
#ifdef SWIFT_DEBUG_CHECKS
/* Check that particles have been drifted to the current time */
if
(
gpi
->
ti_drift
!=
e
->
ti_current
)
error
(
"gpi not drifted to current time"
);
if
(
gpj
->
ti_drift
!=
e
->
ti_current
)
error
(
"gpj not drifted to current time"
);
#endif
/* Interact ! */
runner_iact_grav_pp_nonsym
(
r2
,
dx
,
gpi
,
gpj
);
#ifdef SWIFT_DEBUG_CHECKS
gpi
->
num_interacted
++
;
#endif
}
}
}
/* Loop over all particles in cj... */
if
(
cell_is_active
(
cj
,
e
))
{
for
(
int
pjd
=
0
;
pjd
<
gcount_j
;
pjd
++
)
{
/* Get a hold of the ith part in ci. */
struct
gpart
*
restrict
gpj
=
&
gparts_j
[
pjd
];
if
(
!
gpart_is_active
(
gpj
,
e
))
continue
;
/* Apply boundary condition */
const
double
pjx
[
3
]
=
{
gpj
->
x
[
0
]
+
shift
[
0
],
gpj
->
x
[
1
]
+
shift
[
1
],
gpj
->
x
[
2
]
+
shift
[
2
]};
/* Loop over every particle in the other cell. */
for
(
int
pid
=
0
;
pid
<
gcount_i
;
pid
++
)
{
/* Get a hold of the ith part in ci. */
const
struct
gpart
*
restrict
gpi
=
&
gparts_i
[
pid
];
/* Compute the pairwise distance. */
const
float
dx
[
3
]
=
{
pjx
[
0
]
-
gpi
->
x
[
0
],
// x
pjx
[
1
]
-
gpi
->
x
[
1
],
// y
pjx
[
2
]
-
gpi
->
x
[
2
]};
// z
const
float
r2
=
dx
[
0
]
*
dx
[
0
]
+
dx
[
1
]
*
dx
[
1
]
+
dx
[
2
]
*
dx
[
2
];
#ifdef SWIFT_DEBUG_CHECKS
/* Check that particles have been drifted to the current time */
if
(
gpi
->
ti_drift
!=
e
->
ti_current
)
error
(
"gpi not drifted to current time"
);
if
(
gpj
->
ti_drift
!=
e
->
ti_current
)
error
(
"gpj not drifted to current time"
);
#endif
/* Interact ! */
runner_iact_grav_pp_nonsym
(
r2
,
dx
,
gpj
,
gpi
);
#ifdef SWIFT_DEBUG_CHECKS
gpj
->
num_interacted
++
;
#endif
}
}
}
#endif
}
/**
...
...
@@ -654,7 +554,7 @@ void runner_dopair_grav_pp_truncated(struct runner *r, struct cell *ci,
/* Now do the opposite loop */
if
(
cj_active
)
{
/* Loop over all particles in c
i
... */
/* Loop over all particles in c
j
... */
for
(
int
pjd
=
0
;
pjd
<
gcount_j
;
pjd
++
)
{
/* Skip inactive particles */
...
...
@@ -752,111 +652,6 @@ void runner_dopair_grav_pp_truncated(struct runner *r, struct cell *ci,
/* Write back to the particles */
if
(
ci_active
)
gravity_cache_write_back
(
ci_cache
,
gparts_i
,
gcount_i
);
if
(
cj_active
)
gravity_cache_write_back
(
cj_cache
,
gparts_j
,
gcount_j
);
#ifdef MATTHIEU_OLD_STUFF
/* Some constants */
const
struct
engine
*
const
e
=
r
->
e
;
const
struct
space
*
s
=
e
->
s
;
const
double
cell_width
=
s
->
width
[
0
];
const
double
a_smooth
=
e
->
gravity_properties
->
a_smooth
;
const
double
rlr
=
cell_width
*
a_smooth
;
const
float
rlr_inv
=
1
.
/
rlr
;
/* Cell properties */
const
int
gcount_i
=
ci
->
gcount
;
const
int
gcount_j
=
cj
->
gcount
;
struct
gpart
*
restrict
gparts_i
=
ci
->
gparts
;
struct
gpart
*
restrict
gparts_j
=
cj
->
gparts
;
/* MATTHIEU: Should we use local DP accumulators ? */
/* Loop over all particles in ci... */
if
(
cell_is_active
(
ci
,
e
))
{
for
(
int
pid
=
0
;
pid
<
gcount_i
;
pid
++
)
{
/* Get a hold of the ith part in ci. */
struct
gpart
*
restrict
gpi
=
&
gparts_i
[
pid
];
if
(
!
gpart_is_active
(
gpi
,
e
))
continue
;
/* Apply boundary condition */
const
double
pix
[
3
]
=
{
gpi
->
x
[
0
]
-
shift
[
0
],
gpi
->
x
[
1
]
-
shift
[
1
],
gpi
->
x
[
2
]
-
shift
[
2
]};
/* Loop over every particle in the other cell. */
for
(
int
pjd
=
0
;
pjd
<
gcount_j
;
pjd
++
)
{
/* Get a hold of the jth part in cj. */
const
struct
gpart
*
restrict
gpj
=
&
gparts_j
[
pjd
];
/* Compute the pairwise distance. */
const
float
dx
[
3
]
=
{
pix
[
0
]
-
gpj
->
x
[
0
],
// x
pix
[
1
]
-
gpj
->
x
[
1
],
// y
pix
[
2
]
-
gpj
->
x
[
2
]};
// z
const
float
r2
=
dx
[
0
]
*
dx
[
0
]
+
dx
[
1
]
*
dx
[
1
]
+
dx
[
2
]
*
dx
[
2
];
#ifdef SWIFT_DEBUG_CHECKS
/* Check that particles have been drifted to the current time */
if
(
gpi
->
ti_drift
!=
e
->
ti_current
)
error
(
"gpi not drifted to current time"
);
if
(
gpj
->
ti_drift
!=
e
->
ti_current
)
error
(
"gpj not drifted to current time"
);
#endif
/* Interact ! */
runner_iact_grav_pp_truncated_nonsym
(
r2
,
dx
,
gpi
,
gpj
,
rlr_inv
);
#ifdef SWIFT_DEBUG_CHECKS
gpi
->
num_interacted
++
;
#endif
}
}
}
/* Loop over all particles in cj... */
if
(
cell_is_active
(
cj
,
e
))
{
for
(
int
pjd
=
0
;
pjd
<
gcount_j
;
pjd
++
)
{
/* Get a hold of the ith part in ci. */
struct
gpart
*
restrict
gpj
=
&
gparts_j
[
pjd
];
if
(
!
gpart_is_active
(
gpj
,
e
))
continue
;
/* Apply boundary condition */
const
double
pjx
[
3
]
=
{
gpj
->
x
[
0
]
+
shift
[
0
],
gpj
->
x
[
1
]
+
shift
[
1
],
gpj
->
x
[
2
]
+
shift
[
2
]};
/* Loop over every particle in the other cell. */
for
(
int
pid
=
0
;
pid
<
gcount_i
;
pid
++
)
{
/* Get a hold of the ith part in ci. */
const
struct
gpart
*
restrict
gpi
=
&
gparts_i
[
pid
];
/* Compute the pairwise distance. */
const
float
dx
[
3
]
=
{
pjx
[
0
]
-
gpi
->
x
[
0
],
// x
pjx
[
1
]
-
gpi
->
x
[
1
],
// y
pjx
[
2
]
-
gpi
->
x
[
2
]};
// z
const
float
r2
=
dx
[
0
]
*
dx
[
0
]
+
dx
[
1
]
*
dx
[
1
]
+
dx
[
2
]
*
dx
[
2
];
#ifdef SWIFT_DEBUG_CHECKS
/* Check that particles have been drifted to the current time */
if
(
gpi
->
ti_drift
!=
e
->
ti_current
)
error
(
"gpi not drifted to current time"
);
if
(
gpj
->
ti_drift
!=
e
->
ti_current
)
error
(
"gpj not drifted to current time"
);
#endif
/* Interact ! */
runner_iact_grav_pp_truncated_nonsym
(
r2
,
dx
,
gpj
,
gpi
,
rlr_inv
);
#ifdef SWIFT_DEBUG_CHECKS
gpj
->
num_interacted
++
;
#endif
}
}
}
#endif
}
/**
...
...
@@ -1045,80 +840,6 @@ void runner_doself_grav_pp_full(struct runner *r, struct cell *c) {
/* Write back to the particles */
gravity_cache_write_back
(
ci_cache
,
gparts
,
gcount
);
#ifdef MATTHIEU_OLD_STUFF
/* Some constants */
const
struct
engine
*
const
e
=
r
->
e
;
/* Cell properties */
const
int
gcount
=
c
->
gcount
;
struct
gpart
*
restrict
gparts
=
c
->
gparts
;
/* MATTHIEU: Should we use local DP accumulators ? */
/* Loop over all particles in ci... */
for
(
int
pid
=
0
;
pid
<
gcount
;
pid
++
)
{
/* Get a hold of the ith part in ci. */
struct
gpart
*
restrict
gpi
=
&
gparts
[
pid
];
/* Loop over every particle in the other cell. */
for
(
int
pjd
=
pid
+
1
;
pjd
<
gcount
;
pjd
++
)
{
/* Get a hold of the jth part in ci. */
struct
gpart
*
restrict
gpj
=
&
gparts
[
pjd
];
/* Compute the pairwise distance. */
float
dx
[
3
]
=
{
gpi
->
x
[
0
]
-
gpj
->
x
[
0
],
// x
gpi
->
x
[
1
]
-
gpj
->
x
[
1
],
// y
gpi
->
x
[
2
]
-
gpj
->
x
[
2
]};
// z
const
float
r2
=
dx
[
0
]
*
dx
[
0
]
+
dx
[
1
]
*
dx
[
1
]
+
dx
[
2
]
*
dx
[
2
];
#ifdef SWIFT_DEBUG_CHECKS
/* Check that particles have been drifted to the current time */
if
(
gpi
->
ti_drift
!=
e
->
ti_current
)
error
(
"gpi not drifted to current time"
);
if
(
gpj
->
ti_drift
!=
e
->
ti_current
)
error
(
"gpj not drifted to current time"
);
#endif
/* Interact ! */
if
(
gpart_is_active
(
gpi
,
e
)
&&
gpart_is_active
(
gpj
,
e
))
{
runner_iact_grav_pp
(
r2
,
dx
,
gpi
,
gpj
);
#ifdef SWIFT_DEBUG_CHECKS
gpi
->
num_interacted
++
;
gpj
->
num_interacted
++
;
#endif
}
else
{
if
(
gpart_is_active
(
gpi
,
e
))
{
runner_iact_grav_pp_nonsym
(
r2
,
dx
,
gpi
,
gpj
);
#ifdef SWIFT_DEBUG_CHECKS
gpi
->
num_interacted
++
;
#endif
}
else
if
(
gpart_is_active
(
gpj
,
e
))
{
dx
[
0
]
=
-
dx
[
0
];
dx
[
1
]
=
-
dx
[
1
];
dx
[
2
]
=
-
dx
[
2
];
runner_iact_grav_pp_nonsym
(
r2
,
dx
,
gpj
,
gpi
);
#ifdef SWIFT_DEBUG_CHECKS
gpj
->
num_interacted
++
;
#endif
}
}
}
}
#endif
}
/**
...
...
@@ -1264,83 +985,6 @@ void runner_doself_grav_pp_truncated(struct runner *r, struct cell *c) {
/* Write back to the particles */
gravity_cache_write_back
(
ci_cache
,
gparts
,
gcount
);
#ifdef MATTHIEU_OLD_STUFF
/* Some constants */
const
struct
engine
*
const
e
=
r
->
e
;
const
struct
space
*
s
=
e
->
s
;
const
double
cell_width
=
s
->
width
[
0
];
const
double
a_smooth
=
e
->
gravity_properties
->
a_smooth
;
const
double
rlr
=
cell_width
*
a_smooth
;
const
float
rlr_inv
=
1
.
/
rlr
;
/* Cell properties */
const
int
gcount
=
c
->
gcount
;
struct
gpart
*
restrict
gparts
=
c
->
gparts
;
/* MATTHIEU: Should we use local DP accumulators ? */
/* Loop over all particles in ci... */
for
(
int
pid
=
0
;
pid
<
gcount
;
pid
++
)
{
/* Get a hold of the ith part in ci. */
struct
gpart
*
restrict
gpi
=
&
gparts
[
pid
];
/* Loop over every particle in the other cell. */
for
(
int
pjd
=
pid
+
1
;
pjd
<
gcount
;
pjd
++
)
{
/* Get a hold of the jth part in ci. */
struct
gpart
*
restrict
gpj
=
&
gparts
[
pjd
];
/* Compute the pairwise distance. */
float
dx
[
3
]
=
{
gpi
->
x
[
0
]
-
gpj
->
x
[
0
],
// x
gpi
->
x
[
1
]
-
gpj
->
x
[
1
],
// y
gpi
->
x
[
2
]
-
gpj
->
x
[
2
]};
// z
const
float
r2
=
dx
[
0
]
*
dx
[
0
]
+
dx
[
1
]
*
dx
[
1
]
+
dx
[
2
]
*
dx
[
2
];
#ifdef SWIFT_DEBUG_CHECKS
/* Check that particles have been drifted to the current time */
if
(
gpi
->
ti_drift
!=
e
->
ti_current
)
error
(
"gpi not drifted to current time"
);
if
(
gpj
->
ti_drift
!=
e
->
ti_current
)
error
(
"gpj not drifted to current time"
);
#endif
/* Interact ! */
if
(
gpart_is_active
(
gpi
,
e
)
&&
gpart_is_active
(
gpj
,
e
))
{
runner_iact_grav_pp_truncated
(
r2
,
dx
,
gpi
,
gpj
,
rlr_inv
);
#ifdef SWIFT_DEBUG_CHECKS
gpi
->
num_interacted
++
;
gpj
->
num_interacted
++
;
#endif
}
else
{
if
(
gpart_is_active
(
gpi
,
e
))
{
runner_iact_grav_pp_truncated_nonsym
(
r2
,
dx
,
gpi
,
gpj
,
rlr_inv
);
#ifdef SWIFT_DEBUG_CHECKS
gpi
->
num_interacted
++
;
#endif
}
else
if
(
gpart_is_active
(
gpj
,
e
))
{
dx
[
0
]
=
-
dx
[
0
];
dx
[
1
]
=
-
dx
[
1
];
dx
[
2
]
=
-
dx
[
2
];
runner_iact_grav_pp_truncated_nonsym
(
r2
,
dx
,
gpj
,
gpi
,
rlr_inv
);
#ifdef SWIFT_DEBUG_CHECKS
gpj
->
num_interacted
++
;
#endif
}
}
}
}
#endif
}
/**
...
...
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