Skip to content
GitLab
Explore
Sign in
Primary navigation
Search or go to…
Project
SWIFTsim
Manage
Activity
Members
Labels
Plan
Issues
Issue boards
Milestones
Wiki
Code
Merge requests
Repository
Branches
Commits
Tags
Repository graph
Compare revisions
Snippets
Deploy
Releases
Model registry
Monitor
Incidents
Analyze
Value stream analytics
Contributor analytics
Repository analytics
Model experiments
Help
Help
Support
GitLab documentation
Compare GitLab plans
Community forum
Contribute to GitLab
Provide feedback
Keyboard shortcuts
?
Snippets
Groups
Projects
Show more breadcrumbs
SWIFT
SWIFTsim
Commits
a3ecd167
Commit
a3ecd167
authored
7 years ago
by
James Willis
Browse files
Options
Downloads
Patches
Plain Diff
Use intrinsics in arithmetic operations to support AVX-512 in runner_iact_nonsym_1_force_vec.
parent
02b12046
No related branches found
No related tags found
1 merge request
!406
Doself2 vectorisation
Changes
1
Hide whitespace changes
Inline
Side-by-side
Showing
1 changed file
src/hydro/Gadget2/hydro_iact.h
+29
-37
29 additions, 37 deletions
src/hydro/Gadget2/hydro_iact.h
with
29 additions
and
37 deletions
src/hydro/Gadget2/hydro_iact.h
+
29
−
37
View file @
a3ecd167
...
...
@@ -1169,6 +1169,8 @@ __attribute__((always_inline)) INLINE static void runner_iact_nonsym_vec_force(
}
#ifdef WITH_VECTORIZATION
static
const
vector
const_viscosity_alpha_fac
=
FILL_VEC
(
-
0
.
25
f
*
const_viscosity_alpha
);
__attribute__
((
always_inline
))
INLINE
static
void
runner_iact_nonsym_1_vec_force
(
vector
*
r2
,
vector
*
dx
,
vector
*
dy
,
vector
*
dz
,
vector
vix
,
vector
viy
,
...
...
@@ -1182,7 +1184,7 @@ runner_iact_nonsym_1_vec_force(
#ifdef WITH_VECTORIZATION
vector
r
,
ri
;
vector
vjx
,
vjy
,
vjz
;
vector
vjx
,
vjy
,
vjz
,
dvx
,
dvy
,
dvz
;
vector
pjrho
,
grad_hj
,
pjPOrho2
,
balsara_j
,
cj
,
mj
,
hj_inv
;
vector
xi
,
xj
;
vector
hid_inv
,
hjd_inv
;
...
...
@@ -1209,63 +1211,66 @@ runner_iact_nonsym_1_vec_force(
fac_mu
.
v
=
vec_set1
(
1
.
f
);
/* Will change with cosmological integration */
/* Load stuff. */
balsara
.
v
=
balsara_i
.
v
+
balsara_j
.
v
;
balsara
.
v
=
vec_add
(
balsara_i
.
v
,
balsara_j
.
v
)
;
/* Get the radius and inverse radius. */
ri
=
vec_reciprocal_sqrt
(
*
r2
);
r
.
v
=
r2
->
v
*
ri
.
v
;
r
.
v
=
vec_mul
(
r2
->
v
,
ri
.
v
)
;
/* Get the kernel for hi. */
hid_inv
=
pow_dimension_plus_one_vec
(
hi_inv
);
xi
.
v
=
r
.
v
*
hi_inv
.
v
;
xi
.
v
=
vec_mul
(
r
.
v
,
hi_inv
.
v
)
;
kernel_eval_dWdx_force_vec
(
&
xi
,
&
wi_dx
);
wi_dr
.
v
=
hid_inv
.
v
*
wi_dx
.
v
;
wi_dr
.
v
=
vec_mul
(
hid_inv
.
v
,
wi_dx
.
v
)
;
/* Get the kernel for hj. */
hjd_inv
=
pow_dimension_plus_one_vec
(
hj_inv
);
xj
.
v
=
r
.
v
*
hj_inv
.
v
;
xj
.
v
=
vec_mul
(
r
.
v
,
hj_inv
.
v
)
;
/* Calculate the kernel for two particles. */
kernel_eval_dWdx_force_vec
(
&
xj
,
&
wj_dx
);
wj_dr
.
v
=
hjd_inv
.
v
*
wj_dx
.
v
;
wj_dr
.
v
=
vec_mul
(
hjd_inv
.
v
,
wj_dx
.
v
);
/* Compute dv. */
dvx
.
v
=
vec_sub
(
vix
.
v
,
vjx
.
v
);
dvy
.
v
=
vec_sub
(
viy
.
v
,
vjy
.
v
);
dvz
.
v
=
vec_sub
(
viz
.
v
,
vjz
.
v
);
/* Compute dv dot r. */
dvdr
.
v
=
((
vix
.
v
-
vjx
.
v
)
*
dx
->
v
)
+
((
viy
.
v
-
vjy
.
v
)
*
dy
->
v
)
+
((
viz
.
v
-
vjz
.
v
)
*
dz
->
v
);
dvdr
.
v
=
vec_fma
(
dvx
.
v
,
dx
->
v
,
vec_fma
(
dvy
.
v
,
dy
->
v
,
vec_mul
(
dvz
.
v
,
dz
->
v
)));
/* Compute the relative velocity. (This is 0 if the particles move away from
* each other and negative otherwise) */
omega_ij
.
v
=
vec_fmin
(
dvdr
.
v
,
vec_setzero
());
mu_ij
.
v
=
fac_mu
.
v
*
ri
.
v
*
omega_ij
.
v
;
/* This is 0 or negative */
mu_ij
.
v
=
vec_mul
(
fac_mu
.
v
,
vec_mul
(
ri
.
v
,
omega_ij
.
v
))
;
/* This is 0 or negative */
/* Compute signal velocity */
v_sig
.
v
=
ci
.
v
+
cj
.
v
-
vec_set1
(
3
.
0
f
)
*
mu_ij
.
v
;
v_sig
.
v
=
vec_fnma
(
vec_set1
(
3
.
f
)
,
mu_ij
.
v
,
vec_add
(
ci
.
v
,
cj
.
v
))
;
/* Now construct the full viscosity term */
rho_ij
.
v
=
vec_set1
(
0
.
5
f
)
*
(
pirho
.
v
+
pjrho
.
v
);
visc
.
v
=
vec_set1
(
-
0
.
25
f
)
*
vec_set1
(
const_viscosity_alpha
)
*
v_sig
.
v
*
mu_ij
.
v
*
balsara
.
v
/
rho_ij
.
v
;
rho_ij
.
v
=
vec_mul
(
vec_set1
(
0
.
5
f
),
vec_add
(
pirho
.
v
,
pjrho
.
v
));
visc
.
v
=
vec_div
(
vec_mul
(
const_viscosity_alpha_fac
.
v
,
vec_mul
(
v_sig
.
v
,
vec_mul
(
mu_ij
.
v
,
balsara
.
v
))),
rho_ij
.
v
);
/* Now, convolve with the kernel */
visc_term
.
v
=
vec_set1
(
0
.
5
f
)
*
visc
.
v
*
(
wi_dr
.
v
+
wj_dr
.
v
)
*
ri
.
v
;
sph_term
.
v
=
(
grad_hi
.
v
*
piPOrho2
.
v
*
wi_dr
.
v
+
grad_hj
.
v
*
pjPOrho2
.
v
*
wj_dr
.
v
)
*
ri
.
v
;
visc_term
.
v
=
vec_mul
(
vec_set1
(
0
.
5
f
),
vec_mul
(
visc
.
v
,
vec_mul
(
vec_add
(
wi_dr
.
v
,
wj_dr
.
v
),
ri
.
v
)));
sph_term
.
v
=
vec_mul
(
vec_fma
(
vec_mul
(
grad_hi
.
v
,
piPOrho2
.
v
),
wi_dr
.
v
,
vec_mul
(
grad_hj
.
v
,
vec_mul
(
pjPOrho2
.
v
,
wj_dr
.
v
))),
ri
.
v
);
/* Eventually get the acceleration */
acc
.
v
=
visc_term
.
v
+
sph_term
.
v
;
acc
.
v
=
vec_add
(
visc_term
.
v
,
sph_term
.
v
)
;
/* Use the force, Luke! */
piax
.
v
=
mj
.
v
*
dx
->
v
*
acc
.
v
;
piay
.
v
=
mj
.
v
*
dy
->
v
*
acc
.
v
;
piaz
.
v
=
mj
.
v
*
dz
->
v
*
acc
.
v
;
piax
.
v
=
vec_mul
(
mj
.
v
,
vec_mul
(
dx
->
v
,
acc
.
v
))
;
piay
.
v
=
vec_mul
(
mj
.
v
,
vec_mul
(
dy
->
v
,
acc
.
v
))
;
piaz
.
v
=
vec_mul
(
mj
.
v
,
vec_mul
(
dz
->
v
,
acc
.
v
))
;
/* Get the time derivative for h. */
pih_dt
.
v
=
mj
.
v
*
dvdr
.
v
*
ri
.
v
/
pjrho
.
v
*
wi_dr
.
v
;
pih_dt
.
v
=
vec_div
(
vec_mul
(
mj
.
v
,
vec_mul
(
dvdr
.
v
,
vec_mul
(
ri
.
v
,
wi_dr
.
v
))),
pjrho
.
v
)
;
/* Change in entropy */
entropy_dt
.
v
=
mj
.
v
*
visc_term
.
v
*
dvdr
.
v
;
entropy_dt
.
v
=
vec_mul
(
mj
.
v
,
vec_mul
(
visc_term
.
v
,
dvdr
.
v
))
;
/* Store the forces back on the particles. */
a_hydro_xSum
->
v
=
vec_mask_sub
(
a_hydro_xSum
->
v
,
piax
.
v
,
mask
);
...
...
@@ -1417,9 +1422,6 @@ runner_iact_nonsym_2_vec_force(
rho_ij
.
v
=
vec_mul
(
vec_set1
(
0
.
5
f
),
vec_add
(
pirho
.
v
,
pjrho
.
v
));
rho_ij_2
.
v
=
vec_mul
(
vec_set1
(
0
.
5
f
),
vec_add
(
pirho
.
v
,
pjrho_2
.
v
));
vector
const_viscosity_alpha_fac
;
const_viscosity_alpha_fac
.
v
=
vec_set1
(
-
0
.
25
f
*
const_viscosity_alpha
);
visc
.
v
=
vec_div
(
vec_mul
(
const_viscosity_alpha_fac
.
v
,
vec_mul
(
v_sig
.
v
,
vec_mul
(
mu_ij
.
v
,
balsara
.
v
))),
rho_ij
.
v
);
visc_2
.
v
=
vec_div
(
vec_mul
(
const_viscosity_alpha_fac
.
v
,
vec_mul
(
v_sig_2
.
v
,
vec_mul
(
mu_ij_2
.
v
,
balsara_2
.
v
))),
rho_ij_2
.
v
);
...
...
@@ -1446,16 +1448,6 @@ runner_iact_nonsym_2_vec_force(
piaz
.
v
=
vec_mul
(
mj
.
v
,
vec_mul
(
dz
.
v
,
acc
.
v
));
piaz_2
.
v
=
vec_mul
(
mj_2
.
v
,
vec_mul
(
dz_2
.
v
,
acc_2
.
v
));
// for(int i=0; i<VEC_SIZE; i++) {
// message("mj: %f",mj.f[i]);
// message("dvdr: %f",dvdr.f[i]);
// message("ri: %f",ri.f[i]);
// message("pjrho: %f",pjrho.f[i]);
// message("wi_dr: %f",wi_dr.f[i]);
// message("wi_dx: %f",wi_dx.f[i]);
// message("hid_inv: %f",hid_inv.f[i]);
// }
/* Get the time derivative for h. */
pih_dt
.
v
=
vec_div
(
vec_mul
(
mj
.
v
,
vec_mul
(
dvdr
.
v
,
vec_mul
(
ri
.
v
,
wi_dr
.
v
))),
pjrho
.
v
);
pih_dt_2
.
v
=
vec_div
(
vec_mul
(
mj_2
.
v
,
vec_mul
(
dvdr_2
.
v
,
vec_mul
(
ri_2
.
v
,
wi_dr_2
.
v
))),
pjrho_2
.
v
);
...
...
This diff is collapsed.
Click to expand it.
Preview
0%
Loading
Try again
or
attach a new file
.
Cancel
You are about to add
0
people
to the discussion. Proceed with caution.
Finish editing this message first!
Save comment
Cancel
Please
register
or
sign in
to comment