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Evan Hall
pygwinc
Commits
b23fc66e
Commit
b23fc66e
authored
2 years ago
by
Kevin Kuns
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Merge branch 'budget-tests' into 'master'
Budget tests See merge request
!155
parents
fb790018
df6a16cd
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README.md
+6
-6
6 additions, 6 deletions
README.md
test/budgets/test_budgets.py
+75
-0
75 additions, 0 deletions
test/budgets/test_budgets.py
with
81 additions
and
6 deletions
README.md
+
6
−
6
View file @
b23fc66e
...
...
@@ -153,8 +153,8 @@ is available in the `budget.ifo` attribute.
The budget
`run()`
method calculates all budget noises and the noise
total and returns a
`BudgetTrace`
object with
`freq`
,
`psd`
, and
`asd`
properties. The budget sub-traces are available through a dictionary
(
`trace['Quantum
Vacuum
']`
) interface and via attributes
(
`trace.Quantum
Vacumm
`
).
(
`trace['Quantum']`
) interface and via attributes
(
`trace.Quantum`
).
The budget
`freq`
and
`ifo`
attributes can be updated at run time by
passing them as keyword arguments to the
`run()`
method:
...
...
@@ -438,21 +438,21 @@ and extract the noise data the output traces dictionary:
```
python
budget
=
load_budget
(
'
/path/to/MyBudget
'
,
freq
)
trace
=
budget
.
run
()
quantum_trace
=
trace
[
'
Quantum
Vacuum
'
]
quantum_trace
=
trace
[
'
Quantum
'
]
```
You can also calculate the final calibrated output noise for just a
single term using the Budget
`calc_noise()`
method:
```
python
data
=
budget
.
calc_noise
(
'
Quantum
Vacuum
'
)
data
=
budget
.
calc_noise
(
'
Quantum
'
)
```
You can also calculate a noise at it's source, without applying any
calibrations, by using the Budget
`__getitem__`
interface to extract
the specific Noise BudgetItem for the noise you're interested in, and
running it's
`calc()`
method directly:
running it's
`calc
_trace
()`
method directly:
```
python
data
=
budget
[
'
Quantum
Vacuum
'
].
calc
()
data
=
budget
[
'
Quantum
'
].
calc
_trace
()
```
...
...
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test/budgets/test_budgets.py
+
75
−
0
View file @
b23fc66e
...
...
@@ -5,6 +5,8 @@ import gwinc
from
gwinc
import
load_budget
import
gwinc.io
as
io
from
copy
import
deepcopy
from
gwinc.ifo.noises
import
dhdl
import
matplotlib.pyplot
as
plt
import
pytest
...
...
@@ -47,6 +49,79 @@ def test_sub_budgets(ifo, tpath_join):
fig
.
savefig
(
tpath_join
(
trace
.
name
+
'
.pdf
'
))
@pytest.mark.logic
def
test_budget_run_calc
(
tpath_join
,
pprint
,
compare_noise
):
"""
Tests that
1) budget.run() calculates the entire budget including calibration
2) budget.calc_noise(name) calculates the name sub-budget including calibration
3) budget[name].calc_trace() calculates the name sub-budget not including calibration
4) Both 1) and 2) are still true when called directly on sub-budgets
5) Both budget[name].calc_trace(sub_trace) and budget[name][sub_trace].calc_trace()
calculate the sub_trace trace of the name sub-budget without the calibration
of the main budget
6) budget[name].run() is the same as budget[name].calc_trace()
"""
F_Hz
=
np
.
logspace
(
np
.
log10
(
5
),
4
,
3000
)
B
=
load_budget
(
'
CE2silica
'
,
freq
=
F_Hz
)
traces1
=
B
.
run
()
traces2
=
B
.
calc_noise
(
'
Quantum
'
)
traces3
=
B
[
'
Quantum
'
].
calc_trace
()
traces4
=
B
[
'
Quantum
'
].
calc_noise
(
'
AS
'
)
traces5
=
B
[
'
Quantum
'
][
'
AS
'
].
calc_trace
()
traces6
=
B
[
'
Quantum
'
].
run
()
fig1
=
traces1
.
Quantum
.
plot
()
fig2
=
traces2
.
plot
()
fig3
=
traces3
.
plot
()
fig1
.
savefig
(
tpath_join
(
'
run.pdf
'
))
fig2
.
savefig
(
tpath_join
(
'
calc_noise.pdf
'
))
fig3
.
savefig
(
tpath_join
(
'
calc_trace.pdf
'
))
pprint
(
'
Testing that run() and calc_noise() do the same thing
'
)
compare_noise
(
traces1
.
Quantum
,
traces2
)
compare_noise
(
traces1
.
Quantum
.
AS
,
traces2
.
AS
)
pprint
(
"
Testing that run() and calc_trace() on sub-budgets don
'
t apply strain calibration
"
)
compare_noise
(
traces3
,
traces6
)
def
update_total_psd
(
traces
):
total_psd
=
np
.
sum
([
trace
.
psd
for
trace
in
traces
],
axis
=
0
)
traces
.
_psd
=
total_psd
# divide displacement noise by arm length for ease of plotting
Larm_m
=
B
.
ifo
.
Infrastructure
.
Length
dhdl_sqr
,
sinc_sqr
=
dhdl
(
B
.
freq
,
Larm_m
)
for
trace
in
traces3
:
trace
.
_psd
/=
Larm_m
**
2
update_total_psd
(
traces3
)
fig
,
ax
=
plt
.
subplots
()
ax
.
loglog
(
F_Hz
,
traces1
.
Quantum
.
asd
,
label
=
'
run
'
)
ax
.
loglog
(
F_Hz
,
traces2
.
asd
,
ls
=
'
--
'
,
label
=
'
calc_noise
'
)
ax
.
loglog
(
F_Hz
,
traces3
.
asd
,
ls
=
'
-.
'
,
label
=
'
calc_trace / $L_\mathrm{arm}$
'
)
# convert displacement noise into strain
for
trace
in
traces3
:
trace
.
_psd
*=
sinc_sqr
update_total_psd
(
traces3
)
ax
.
loglog
(
F_Hz
,
traces3
.
asd
,
ls
=
'
:
'
,
label
=
'
calc_trace / $(\mathrm{d}h/\mathrm{d}L_\mathrm{arm})$
'
)
ax
.
set_xlim
(
F_Hz
[
0
],
F_Hz
[
-
1
])
ax
.
grid
(
True
,
which
=
'
major
'
,
alpha
=
0.5
)
ax
.
grid
(
True
,
which
=
'
minor
'
,
alpha
=
0.2
)
ax
.
set_xlabel
(
'
Frequency [Hz]
'
)
ax
.
set_ylabel
(
'
Strain noise [1/Hz$^{-1/2}$]
'
)
ax
.
legend
()
fig
.
savefig
(
tpath_join
(
'
comparison.pdf
'
))
pprint
(
'
Testing that calc_trace() is the same as calc_noise() without calibration
'
)
compare_noise
(
traces2
,
traces3
)
pprint
(
'
Testing that calc_noise() and calc_trace() on sub-budgets are right
'
)
compare_noise
(
traces4
,
traces5
)
@pytest.mark.logic
@pytest.mark.fast
def
test_update_ifo_struct
():
...
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