4 | Introduction - LG LS091HSV3 Engineering Manual

Single zone high efficiency, standard and extended pipe wall mount
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Table 38: Linear Thermal Expansion of Copper Tubing in Inches.
Pipe
Length
1
35°
40°
45°
10
0.04
0.04
0.05
20
0.08
0.08
0.10
30
0.12
0.12
0.15
40
0.16
0.16
0.20
50
0.20
0.20
0.25
60
0.24
0.24
0.30
Pipe length baseline temperature = 0°F. "Expansion of Carbon, Copper and Stainless Steel Pipe," The Engineers' Toolbox, www.engineeringtoolbox.com.
1
Figure 30: Coiled Expansion Loops and Offsets.
L
R
Large Tubing U-bend (>3/4 in.)
Table 39: Radii of Coiled Expansion Loops and Developed Lengths of Expansion Offsets.
Anticipated Linear
Expansion (LE) (inches)
R
1
1/2
L
2
R
1
1
L
2
R
1
1-1/2
L
2
R
1
2
L
2
R
1
2-1/2
L
2
R
1
3
L
2
R
1
3-1/2
L
2
R
1
4
L
2
R = Centerline Length of Pipe.
1
L = Centerline Minimum Radius (inches).
2
50°
55°
60°
65°
70°
0.06
0.06
0.07
0.08
0.08
0.12
0.13
0.14
0.15
0.16
0.18
0.20
0.21
0.23
0.24
0.24
0.26
0.28
0.30
0.32
0.30
0.33
0.35
0.38
0.40
0.36
0.39
0.42
0.45
0.48
L
Nominal Tube Size (OD) inches
1/4
3/8
6
7
38
44
9
10
54
63
11
12
66
77
12
14
77
89
14
16
86
99
15
17
94
109
16
19
102
117
17
20
109
126
Due to our policy of continuous product innovation, some specifications may change without notification.
©
LG Electronics U.S.A., Inc., Englewood Cliffs, NJ. All rights reserved. "LG " is a registered trademark of LG Corp.
REFRIGERANT PIPING DESIGN
Selecting Field-Supplied Copper Tubing
Fluid Temperature °F
75°
80°
85°
90°
95° 100° 105° 110° 115° 120° 125° 130°
0.09
0.09
0.10
0.10
0.11
0.17
0.18
0.19
0.20
0.21
0.26
0.27
0.29
0.30
0.32
0.34
0.36
0.38
0.40
0.42
0.43
0.45
0.48
0.50
0.53
0.51
0.54
0.57
0.60
0.63
R
Loop
1/2
3/4
8
9
50
59
11
13
70
83
14
16
86
101
16
19
99
117
18
21
111
131
19
23
122
143
21
25
131
155
22
26
140
166
0.11
0.11
0.12
0.13
0.14
0.22
0.22
0.23
0.26
0.28
0.33
0.32
0.35
0.39
0.42
0.44
0.43
0.46
0.52
0.56
0.55
0.54
0.58
0.65
0.70
0.66
0.65
0.69
0.78
0.84
L
Small Tubing U-bend (<3/4 in.)
REFRIGERANT DESIGN | 65
0.15
0.15
0.29
0.30
0.44
0.45
0.58
0.60
0.73
0.75
0.87
0.90

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