The refractive index of water at 20 °C for visible light is 1.33.[1] The refractive index of normal ice is 1.31 (from List of refractive indices). In general, an index of refraction is a complex number with real and imaginary parts, where the latter indicates the strength of absorption loss at a particular wavelength. In the visible part of the electromagnetic spectrum, the imaginary part of the refractive index is very small. However, water and ice absorb in infrared and close the infrared atmospheric window, thereby contributing to the greenhouse effect.
Over the wavelengths from 0.2 μm to 1.2 μm, and over temperatures from −12 °C to 500 °C, the real part of the index of refraction of water can be calculated by the following empirical expression:[2]
Where:
,
, and
and the appropriate constants are
= 0.244257733, = 0.00974634476, = −0.00373234996, = 0.000268678472, = 0.0015892057, = 0.00245934259, = 0.90070492, = −0.0166626219, = 273.15 K, = 1000 kg/m3, = 589 nm, = 5.432937, and = 0.229202.
In the above expression, T is the absolute temperature of water (in K), is the wavelength of light in nm, is the density of the water in kg/m3, and n is the real part of the index of refraction of water.
Volumic mass of water
In the above formula, the density of water also varies with temperature and is defined by:[3][4]
with:
= −3.983035 °C
= 301.797 °C
= 522528.9 °C2
= 69.34881 °C
= 999.974950 kg / m3
Refractive index (real and imaginary parts) for liquid water
Refractive Index of Liquid Water
Wavelength (μm)
Wavenumber (cm−1)
Frequency (THz)
n
k
α' (cm−1)
0.200
5.00×104
1.50×103
1.396
1.1×10−7
0.069
0.225
4.44×104
1.33×103
1.373
4.9×10−8
0.027
0.250
4.00×104
1.20×103
1.362
3.35×10−8
0.0168
0.275
3.64×104
1.09×103
1.354
2.35×10−8
0.0107
0.300
3.33×104
999
1.349
1.6×10−8
6.7×10−3
0.325
3.08×104
922
1.346
1.08×10−8
4.18×10−3
0.350
2.86×104
857
1.343
6.5×10−9
2.3×10−3
0.375
2.67×104
799
1.341
3.5×10−9
1.2×10−3
0.400
2.50×104
749
1.339
1.86×10−9
5.84×10−4
0.425
2.35×104
705
1.338
1.3×10−9
3.8×10−4
0.450
2.22×104
666
1.337
1.02×10−9
2.85×10−4
0.475
2.11×104
631
1.336
9.35×10−10
2.47×10−4
0.500
2.00×104
600
1.335
1.00×10−9
2.51×10−4
0.525
1.90×104
571
1.334
1.32×10−9
3.16×10−4
0.550
1.82×104
545
1.333
1.96×10−9
4.48×10−4
0.575
1.74×104
521
1.333
3.60×10−9
7.87×10−4
0.600
1.67×104
500
1.332
1.09×10−8
2.28×10−3
0.625
1.60×104
480
1.332
1.39×10−8
2.79×10−3
0.650
1.54×104
461
1.331
1.64×10−8
3.17×10−3
0.675
1.48×104
444
1.331
2.23×10−8
4.15×10−3
0.700
1.43×104
428
1.331
3.35×10−8
6.01×10−3
0.725
1.38×104
414
1.330
9.15×10−8
0.0159
0.750
1.33×104
400
1.330
1.56×10−7
0.0261
0.775
1.29×104
387
1.330
1.48×10−7
0.0240
0.800
1.25×104
375
1.329
1.25×10−7
0.0196
0.825
1.21×104
363
1.329
1.82×10−7
0.0282
0.850
1.18×104
353
1.329
2.93×10−7
0.0433
0.875
1.14×104
343
1.328
3.91×10−7
0.0562
0.900
1.11×104
333
1.328
4.86×10−7
0.0679
0.925
1.08×104
324
1.328
1.06×10−6
0.144
0.950
1.05×104
316
1.327
2.93×10−6
0.388
0.975
1.03×104
307
1.327
3.48×10−6
0.449
1.0
1.0×104
300
1.327
2.89×10−6
0.36
1.2
8300
250
1.324
9.89×10−6
1.0
1.4
7100
210
1.321
1.38×10−4
12
1.6
6200
190
1.317
8.55×10−5
6.7
1.8
5600
170
1.312
1.15×10−4
8.0
2.0
5000
150
1.306
1.1×10−3
69
2.2
4500
136
1.296
2.89×10−4
17
2.4
4200
125
1.279
9.56×10−4
50.
2.6
3800
115
1.242
3.17×10−3
150
2.65
3770
113
1.219
6.7×10−5
318
2.70
3700
111
1.188
0.019
880
2.75
3640
109
1.157
0.059
2700
2.80
3570
107
1.142
0.115
5160
2.85
3510
105
1.149
0.185
8160
2.90
3450
103
1.201
0.268
11600
2.95
3390
102
1.292
0.298
12700
3.00
3330
100.
1.371
0.272
11400
3.05
3280
98.3
1.426
0.240
9990
3.10
3230
96.7
1.467
0.192
7780
3.15
3170
95.2
1.483
0.135
5390
3.20
3120
93.7
1.478
0.0924
3630
3.25
3080
92.2
1.467
0.0610
2360
3.30
3030
90.8
1.450
0.0368
1400
3.35
2990
89.5
1.432
0.0261
979
3.40
2940
88.2
1.420
0.0195
721
3.45
2900
86.9
1.410
0.0132
481
3.50
2860
85.7
1.400
0.0094
340
3.6
2780
83
1.385
0.00515
180
3.7
2700
81
1.374
0.00360
120
3.8
2630
79
1.364
0.00340
110
3.9
2560
77
1.357
0.00380
120
4.0
2500
75
1.351
0.00460
140
4.1
2440
73
1.346
0.00562
170
4.2
2380
71
1.342
0.00688
210
4.3
2330
70.
1.338
0.00845
250
4.4
2270
69
1.334
0.0103
290
4.5
2220
67
1.332
0.0134
370
4.6
2170
65
1.330
0.0147
400
4.7
2130
64
1.330
0.0157
420
4.8
2080
62
1.330
0.0150
390
4.9
2040
61
1.328
0.0137
350
5.0
2000
60.
1.325
0.0124
310
5.1
1960
59
1.322
0.0111
270
5.2
1920
58
1.317
0.0101
240
5.3
1890
57
1.312
0.0098
230
5.4
1850
56
1.305
0.0103
240
5.5
1820
55
1.298
0.0116
380
5.6
1790
54
1.289
0.0142
320
5.7
1750
53
1.277
0.0203
450
5.8
1720
52
1.262
0.0330
710
5.9
1690
51
1.248
0.0622
1300
6.0
1670
50.
1.265
0.107
2200
6.1
1640
49
1.319
0.131
2700
6.2
1610
48.4
1.363
0.0880
1800
6.3
1590
47.6
1.357
0.0570
1100
6.4
1560
46.8
1.347
0.0449
880
6.5
1540
46.1
1.339
0.0392
760
6.6
1520
45.4
1.334
0.0356
680
6.7
1490
44.7
1.329
0.0337
630
6.8
1470
44.1
1.324
0.0327
600
6.9
1450
43.4
1.321
0.0322
590
7.0
1430
42.8
1.317
0.0320
570
The total refractive index of water is given as m = n + ik. The absorption coefficient α' is used in the Beer–Lambert law with the prime here signifying base e convention. Values are for water at 25 °C, and were obtained through various sources in the cited literature review.[5]
R. M. Pope and E. S. Fry, Absorption spectrum (380-700 nm) of pure water. II. Integrating cavity measurements, Appl. Opt., 36, 8710-8723, 1997.
Mobley, Curtis D., Light and water: radiative transfer in natural waters; based in part on collaborations with Rudolph W. Preisendorfer, San Diego, Academic Press, 1994, 592 p., ISBN0-12-502750-8