Goodman DSXC160481B*, Техническое руководство

Страница: 47 / 56

47
COOLING PERFORMANCE DATA
DSXC160361A*-HIGH STAGE
EXPA
NDED
P
E
R
F
O
R
M
A
NCE DA
T
A
CO
OL
IN
G
O
P
ER
A
T
IO
N
M
O
D
E
L
: D
S
X
C
16
03
6
1
A
* /
C
A
*F
37
43*6*
*+
T
X
V
+
M
B
V
C
16
00
**
-1
*
O
ut
door
A
m
bi
e
nt
Te
m
p
er
a
tur
e
65
75
85
9
5
10
5
1
15
E
nt
e
ri
ng I
ndoor
W
e
t
B
u
lb
Te
m
p
e
ra
tur
e
ID
B
*
A
ir
flo
w
59
6
3
67
71
59
6
3
6
7
71
5
9
6
3
6
7
71
5
9
63
6
7
71
59
63
67
71
59
63
67
71
M
B
h
3
1.
8
32
.5
3
4.
7
3
7.
1
3
1.
1
31
.7
33
.9
36.
3
30
.3
31
.0
33
.1
35
.4
29
.6
3
0.
2
32
.3
3
4.
5
2
8.
1
2
8.
7
3
0.
7
3
2.
8
2
6.
0
2
6.
6
2
8.
4
3
0.
4
S/
T
0.
84
0.
79
0.
64
0.
48
0.
87
0.
82
0.
67
0.
50
0.
89
0.
84
0.
68
0.
51
0.
92
0.
86
0.
70
0.
53
0.
96
0.
90
0.
73
0.
55
0.
97
0.
91
0.
74
0.
55
D
e
lta
T
24
2
3
201
6
25
2
4
2
1
16
2
5
2
4
2
1
1
6
2
5
24
2
1
172
52
42
01
62
32
21
91
5
10
06
K
W
2.
13
2.
17
2.
24
2.
32
2.
30
2.
35
2.
43
2.
51
2.
45
2.
50
2.
59
2.
67
2.
58
2.
64
2.
73
2.
82
2.
69
2.
75
2.
85
2.
95
2.
79
2.
85
2.
95
3.
05
A
M
P
S
8.5
8
.7
9
.0
9.
4
9
.2
9
.4
9
.8
10
.1
10
.0
10
.3
10
.6
11
.0
10
.7
1
1.0
11
.4
1
1.8
1
1.4
1
1.7
1
2.
1
1
2.
6
1
2.
1
1
2.
4
1
2.
9
1
3.
4
HI
P
R
22
0
23
7
2
50
2
61
2
47
2
66
2
81
29
3
28
1
30
2
31
9
33
3
32
0
3
44
3
64
3
79
36
0
388
40
9
427
39
8
428
45
2
47
2
LO
P
R
10
3
10
9
1
19
1
27
1
09
1
16
1
26
13
4
11
3
12
0
13
1
14
0
11
9
1
26
1
38
1
47
12
4
132
14
4
154
12
9
137
14
9
15
9
M
B
h
3
4.
5
35.
2
3
7.
6
4
0.
2
3
3.
7
34.
4
36.
8
39
.3
32
.9
33.
6
35.
9
38.
4
32.
1
3
2.
8
35
.0
37
.4
30
.5
31
.1
33
.3
35
.5
28
.2
28
.8
30
.8
32
.9
S/
T
0
.8
7
0.
82
0
.6
7
0
.5
0
0
.90
0.
85
0.
69
0.
5
2
0.
93
0.
8
7
0.
7
1
0.
5
3
0.
96
0
.9
0
0.
73
0.
55
0.
99
0.
93
0.
76
0.
57
1.
00
0.
94
0.
76
0.
57
D
e
lta
T
24
2
3
20
16
24
2
32
0
16
2
4
2
3
2
01
62
5
23
2
0
16
24
23
20
16
23
22
19
15
80
11
50
K
W
2.
18
2.
23
2.
30
2.
38
2.
36
2.
41
2.
49
2.
57
2.
51
2.
57
2.
65
2.
75
2.
65
2.
71
2.
80
2.
90
2.
76
2.
83
2.
92
3.
03
2.
86
2.
93
3.
03
3.
14
A
M
P
S
8.
8
9.
0
9
.3
9.
6
9
.5
9.
7
10.
0
10
.4
10
.3
10.
6
10.
9
11.
3
11.
0
1
1.
3
11
.7
12
.2
11
.8
12
.1
12
.5
13
.0
12
.5
12
.8
13
.2
13
.7
HI
P
R
22
7
244
25
8
2
69
25
5
2
74
29
0
302
29
0
312
32
9
343
33
0
3
55
37
5
3
91
37
1
40
0
42
2
44
0
41
0
44
1
46
6
48
6
LO
P
R
10
6
113
12
3
1
31
11
2
1
19
13
0
139
11
6
124
13
5
144
12
2
1
30
14
2
1
51
12
8
13
6
14
9
15
8
13
3
14
1
15
4
16
4
M
B
h
3
5.
5
36
.3
3
8.
8
4
1.
4
3
4.
7
35
.4
37
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40.
5
33
.8
34
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37
.0
39
.5
33
.0
3
3.
7
36
.1
3
8.
5
3
1.
4
3
2.
1
3
4.
2
3
6.
6
2
9.
1
2
9.
7
3
1.
7
3
3.
9
S/
T
0.
91
0.
86
0.
70
0.
52
0.
95
0.
89
0.
72
0.
54
1.
00
0.
91
0.
74
0.
55
1.
00
0.
94
0.
77
0.
57
1.
00
1.
00
0.
79
0.
59
1.
00
1.
00
0.
80
0.
60
D
e
lta
T
23
2
2
191
5
23
2
2
1
9
16
2
4
2
2
1
9
1
6
2
3
23
2
0
162
22
31
91
52
12
11
81
4
12
94
K
W
2.
20
2.
25
2.
32
2.
40
2.
38
2.
43
2.
51
2.
60
2.
53
2.
59
2.
68
2.
77
2.
67
2.
73
2.
82
2.
92
2.
79
2.
85
2.
95
3.
05
2.
89
2.
96
3.
06
3.
16
A
M
P
S
8.
8
9
.1
9
.4
9.
7
9
.6
9
.8
10
.1
10.
5
10
.4
10
.7
11
.0
11
.5
11
.1
1
1.
4
11
.8
1
2.
3
1
1.
9
1
2.
2
1
2.
6
1
3.
1
1
2.
6
1
2.
9
1
3.
4
1
3.
9
HI
P
R
22
9
24
7
2
61
2
72
2
57
2
77
2
92
30
5
29
3
31
5
33
3
34
7
33
3
3
59
3
79
3
95
37
5
404
42
6
444
41
4
446
47
1
49
1
LO
P
R
10
7
11
4
1
24
1
32
1
13
1
20
1
31
14
0
11
8
12
5
13
7
14
5
12
3
1
31
1
43
1
53
12
9
138
15
0
160
13
4
142
15
5
16
6
M
B
h
3
2.
4
33
.0
3
4.
6
3
6.
9
3
1.
6
32
.2
33
.8
36.
0
30
.9
31
.5
32
.9
35
.1
30
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3
0.
7
32
.1
3
4.
3
2
8.
6
2
9.
2
3
0.
5
3
2.
6
2
6.
5
2
7.
0
2
8.
3
3
0.
2
S/
T
0.
88
0.
85
0.
77
0.
62
0.
91
0.
88
0.
80
0.
65
0.
94
0.
90
0.
82
0.
66
0.
97
0.
93
0.
84
0.
68
1.
00
0.
97
0.
87
0.
71
1.
00
0.
98
0.
88
0.
71
D
e
lta
T
26
2
6
242
1
26
2
6
2
5
21
2
6
2
6
2
5
2
1
2
7
26
2
5
212
62
62
42
12
42
42
32
0
10
06
K
W
2.
14
2.
19
2.
26
2.
34
2.
32
2.
37
2.
45
2.
53
2.
47
2.
52
2.
61
2.
70
2.
60
2.
66
2.
75
2.
85
2.
71
2.
78
2.
87
2.
97
2.
81
2.
88
2.
98
3.
08
A
M
P
S
8.6
8
.8
9
.1
9.
4
9
.3
9
.5
9
.8
10
.2
10
.1
10
.4
10
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11
.1
10
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1
1.1
11
.5
1
1.9
1
1.5
1
1.8
1
2.
2
1
2.
7
1
2.
2
1
2.
5
1
3.
0
1
3.
5
H
I P
R
22
2
23
9
2
53
2
64
2
50
2
69
2
84
29
6
28
4
30
5
32
3
33
6
32
3
3
48
3
67
3
83
36
4
391
41
3
431
40
2
432
45
7
47
6
LO
P
R
10
4
11
0
1
21
1
28
1
10
1
17
1
27
13
6
11
4
12
1
13
2
14
1
12
0
1
27
1
39
1
48
12
6
134
14
6
155
13
0
138
15
1
16
1
M
B
h
3
5.
1
35
.7
3
7.
4
3
9.
9
3
4.
3
34
.9
36
.6
39.
0
33
.4
34
.1
35
.7
38
.1
32
.6
3
3.
3
34
.8
3
7.
2
3
1.
0
3
1.
6
3
3.
1
3
5.
3
2
8.
7
2
9.
3
3
0.
6
3
2.
7
S
/T
0
.9
1
0.
88
0
.8
0
0
.6
5
0
.9
5
0.
91
0.
82
0.6
7
0.
97
0.9
4
0.8
5
0.6
9
1.
00
0
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7
0.
87
0
.7
1
1
.0
0
1
.0
0
0
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1
0
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4
1
.0
0
1
.0
0
0
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1
0
.7
4
D
e
lta
T
26
2
5
242
1
26
2
6
2
4
21
2
6
2
6
2
4
2
1
2
6
26
2
4
212
52
52
42
12
32
32
21
9
85
11
50
K
W
2.
20
2.
25
2.
32
2.
40
2.
38
2.
43
2.
51
2.
60
2.
53
2.
59
2.
68
2.
77
2.
67
2.
73
2.
82
2.
92
2.
79
2.
85
2.
95
3.
05
2.
89
2.
96
3.
06
3.
16
A
M
P
S
8.
8
9
.1
9
.4
9.
7
9
.6
9
.8
10
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10.
5
10
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10
.7
11
.0
11
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11
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1
1.
4
11
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1
2.
3
1
1.
9
1
2.
2
1
2.
6
1
3.
1
1
2.
6
1
2.
9
1
3.
4
1
3.
9
HI
P
R
22
9
24
7
2
61
2
72
2
57
2
77
2
92
30
5
29
3
31
5
33
3
34
7
33
3
3
59
3
79
3
95
37
5
404
42
6
444
41
4
446
47
1
49
1
LO
P
R
10
7
11
4
1
24
1
32
1
13
1
20
1
31
14
0
11
8
12
5
13
7
14
5
12
3
1
31
1
43
1
53
12
9
138
15
0
160
13
4
142
15
5
16
6
M
B
h
3
6.
1
36
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3
8.
6
4
1.
1
3
5.
3
36
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37
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40.
2
34
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35
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36
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39
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33
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3
4.
2
35
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3
8.
3
3
1.
9
3
2.
5
3
4.
1
3
6.
4
2
9.
6
3
0.
1
3
1.
6
3
3.
7
S/
T
0.
96
0.
92
0.
83
0.
68
0.
99
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96
0.
86
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70
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98
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89
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72
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92
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74
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95
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77
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96
0.
78
D
e
lta
T
25
2
4
232
0
25
2
4
2
3
20
2
4
2
5
2
3
2
0
2
4
24
2
3
202
32
32
32
02
12
12
11
9
12
94
K
W
2.
22
2.
27
2.
34
2.
42
2.
40
2.
45
2.
53
2.
62
2.
55
2.
61
2.
70
2.
79
2.
69
2.
75
2.
85
2.
95
2.
81
2.
88
2.
98
3.
08
2.
91
2.
98
3.
08
3.
19
A
M
P
S
8.
9
9
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9
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9.
8
9
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9
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10
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10.
6
10
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10
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11
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11
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11
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1
1.
5
11
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1
2.
4
1
2.
0
1
2.
3
1
2.
7
1
3.
2
1
2.
7
1
3.
0
1
3.
5
1
4.
0
HI
P
R
23
2
24
9
2
63
2
75
2
60
2
80
2
95
30
8
29
6
31
8
33
6
35
0
33
7
3
62
3
83
3
99
37
9
408
43
0
449
41
8
450
47
5
49
6
LO
P
R
10
8
11
5
1
26
1
34
1
14
1
22
1
33
14
1
11
9
12
6
13
8
14
7
12
5
1
33
1
45
1
54
13
1
139
15
2
162
13
5
144
15
7
16
7
*
E
nt
e
rin
g I
nd
oor
D
ry
B
u
lb
T
e
m
pe
ra
tu
re
N
O
TE
:
S
h
ad
e
d
ar
ea
is
A
H
R
I
R
a
tin
g
C
on
di
tio
n
s
K
W
=
T
ot
al
s
ys
tem
p
ow
er
Hi
gh a
n
d
lo
w
p
re
ss
u
res
ar
e m
eas
ur
ed
at
th
e
liq
ui
d
an
d s
u
ct
io
n
s
e
rv
ic
e
v
al
ves
.
A
MP
S
=o
ut
do
o
r u
n
it a
m
p
s
(co
m
p
.+
fa
n
)
HI
GH
S
T
A
G
E