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The
Observed Properties of Liquid Helium
at the Saturated Vapor
Pressure
Chapter 8. Entropy
Adopted
Database
Author(s) |
Key # |
Method |
Range (K) |
Singsass
Table 1 |
1 |
Fountain Pressure |
1.59
T
2.1705 |
Van
den Meijdenberg et al. |
2 |
Fountain Pressure |
1.15
T
2.05 |
Singsass
Table 4 |
3 |
Fountain Pressure |
2.15
T
2.168 |
Singsass
Table 2 |
4 |
Fountain Pressure |
1.6
T
2.159 |
Singsass
Table 5 |
5 |
Fountain Pressure |
(T-T)/T
= 0.1007 to 0.00970 |
Comments and Key to Authors
1,3,4,5)
Singsass and Ahlers; Tables from Singsass Thesis, Ref. 7.
2) Ref. 4.
6) The spline has been adjusted to agree approximately with Singsass and
Ahlers at the lambda point. The spline returns =1.579 J/g.K and =3.025
J/g.K2.
7) Uncertainties: Singsass and Ahlers quote 0.1% precision, 0.5% accuracy.
Van den Meijdenberg et al. quote 1% precision, 3% accuracy.
8) Following the fountain pressure entropy spline are the knots and coefficients
of the fit to entropy data integrated from the recommended values of heat
capacity by
This
spline fit provides entropy data over both helium I and helium II regions.
9) Most heat capacity measurements are reported in Joules/mol.K. Entropy,
however is usually quoted in gram units. To convert data from J/g.K to
J/mol.K multiply by 4.0026. To convert from J/g.K to J/kg.K multiply by
1000.
Table 8.1. Adopted database for the fountain pressure entropy of liquid 4He.
T90 (K) |
Cs (J/mol·K) |
Key |
T90 |
u1 (m/s) |
Key |
1.15302927 |
3.950000E-2 |
2 |
1.90415059 |
7.320000E-1 |
2 |
1.20326685 |
5.150000E-2 |
2 |
1.90415059 |
7.356230E-1 |
4 |
1.25320267 |
6.650000E-2 |
2 |
1.95418895 |
8.420000E-1 |
2 |
1.30332399 |
8.550000E-2 |
2 |
1.95418895
|
8.472770E-1 |
4 |
1.35344288 |
1.075000E-1 |
2 |
2.00303241 |
9.663170E-1 |
1 |
1.40351505 |
1.325000E-1 |
2 |
2.00423358 |
9.630000E-1 |
2 |
1.45355661 |
1.620000E-1 |
2 |
2.00423358 |
9.711100E-1 |
4 |
1.50359791 |
1.960000E-1 |
2 |
2.05429341 |
1.105000E+0
|
2 |
1.55363712
|
2.370000E-1 |
2 |
2.05429341
|
1.113220E+0 |
4 |
1.59708138 |
2.812150E-1 |
1 |
2.10389749
|
1.271440E+0 |
1 |
1.60369037
|
2.840000E-1 |
2 |
2.10439892 |
1.275540E+0 |
4 |
1.60369037 |
2.900930E-1 |
4 |
2.15456275
|
1.468060E+0 |
4 |
1.65377936 |
3.370000E-1 |
2 |
2.15466305
|
1.469430E+0 |
1 |
1.65377936 |
3.425750E-1 |
4 |
2.15469110
|
1.469300E+0 |
3 |
1.69937308 |
3.977850E-1 |
1 |
2.16429053 |
1.512190E+0 |
1 |
1.70388228 |
3.980000E-1 |
2 |
2.16429053 |
1.513560E+0 |
4 |
1.70388228 |
4.034210E-1 |
4
|
2.16429267 |
1.511520E+0 |
3 |
1.75398060 |
4.660000E-1 |
2 |
2.16970354 |
1.540000E+0 |
3 |
1.75408079 |
4.725490E-1 |
4 |
2.16970398 |
1.540690E+0 |
1 |
1.80106080 |
5.449310E-1 |
1 |
2.17290000 |
1.557640E+0 |
1 |
1.80406509
|
5.450000E-1 |
2 |
2.17290343 |
1.557990E+0 |
3 |
1.80406509 |
5.502870E-1 |
4 |
2.17460000 |
1.570540E+0 |
1 |
1.85411884 |
6.330000E-1 |
2
|
2.17510000 |
1.571870E+0 |
1 |
1.85411884 |
6.381940E-1 |
4 |
2.17530000
|
1.573910E+0 |
1 |
1.90214931 |
7.301360E-1
|
1 |
2.17680000 |
1.578970E+0
|
5 |
Figure 8.1. The recommended
values of the fountain pressure entropy of liquid 4He as a function of
temperature at saturated vapor pressure.
Table 8.2. Knots and coefficients
for the spline fit of the fountain pressure entropy.
Knots |
Coefficients |
K(1)
= 1.153029 |
C(1)
= 3.949990E-2 |
K(2)
= 1.153029 |
C(2) = 5.660103E-2 |
K(3)
= 1.153029 |
C(3)
= 9.933250E-2 |
K(4)
= 1.153029 |
C(4)
= 2.321544E-1 |
K(5)
= 1.402666 |
C(5)
= 5.183673E-1 |
K(6)
= 1.501863 |
C(6)
= 9.994261E-1 |
K(7)
= 1.801948 |
C(7)
= 1.506163E+0 |
K(8)
= 2.154592 |
C(8)
= 1.549628E+0 |
K(9)
= 2.164268 |
C(9)
= 1.575018E+0 |
K(10)
= 2.172874 |
C(10)
= 1.578977E+0 |
K(11)
= 2.176800 |
|
K(12)
= 2.176800 |
|
K(13)
= 2.176800 |
|
K(14)
= 2.176800 |
|
Figure 8.2. The fractional
deviation of values of the adopted database from the recommended values
for the fountain pressure entropy of liquid 4He expressed in percent.
Table
8.3. Recommended values of the fountain pressure entropy of liquid 4He.
T90 (K) |
S (J/g K) |
1.20
|
5.059E-2 |
1.25
|
6.560E-2 |
1.30
|
8.397E-2 |
1.35
|
1.057E-1 |
1.40 |
1.310E-1 |
1.45 |
1.600E-1 |
1.50
|
1.940E-1 |
1.55
|
2.343E-1 |
1.60
|
2.815E-1 |
1.65
|
3.357E-1 |
1.70
|
3.972E-1 |
1.75
|
4.662E-1 |
1.80
|
5.429E-1 |
1.85
|
6.279E-1 |
1.90
|
7.233E-1 |
1.95 |
8.319E-1 |
2.00 |
9.561E-1 |
2.05
|
1.099E+0 |
2.10
|
1.262E+0 |
2.15
|
1.450E+0 |
2.1761 |
1.577E+0 |
2.1762 |
1.577E+0 |
2.1763 |
1.577E+0 |
2.1764
|
1.578E+0 |
2.1765
|
1.578E+0 |
2.1766
|
1.578E+0 |
2.1767
|
1.579E+0 |
2.1768
|
1.579E+0 |
Figure 8.3. The recommended
values of the entropy of liquid 4He obtained by integration of the heat
capacity spline.
Table 8.4. Knots and coefficients
for the spline fit of entropy integrated from the recommended values of
heat capacity.
Knots |
Coefficients |
K(1)
= 0.10000 |
C(1)
= 6.60E-6 |
K(2)
= 0.10000 |
C(2)
= 7.60E-6 |
K(3)
= 0.10000 |
C(3)
= 1.60E-5 |
K(4)
= 0.10000 |
C(4)
= 4.61413E-5 |
K(5)
= 0.11123 |
C(5) = 1.8400E-4 |
K(6)
= 0.21625 |
C(6)
= 4.68675E-4 |
K(7)
= 0.27672 |
C(7)
= 0.00121 |
K(8)
= 0.44817 |
C(8) = 0.00236 |
K(9)
= 0.56369 |
C(9)
= 0.00561 |
K(10)
= 0.71969 |
C(10)
= 0.01978 |
K(11)
= 0.85360 |
C(11)
= 0.08337 |
K(12)
= 1.00186 |
C(12)
= 0.35824 |
K(13)
= 1.40184 |
C(13)
= 0.76882 |
K(14)
= 1.72912 |
C(14) = 1.17803 |
K(15)
= 1.99887 |
C(15)
= 1.38629 |
K(16)
= 2.07775 |
C(16)
= 1.53613 |
K(17)
= 2.15384 |
C(17) = 1.58271 |
K(18)
= 2.17680 |
C(18)
= 1.62419 |
K(19)
= 2.17680 |
C(19) = 1.72261 |
K(20)
= 2.17680 |
C(20)
= 1.91862 |
K(21)
= 2.21160 |
C(21)
= 2.53529 |
K(22)
= 2.34820 |
C(22) = 3.16601 |
K(23)
= 2.69075 |
C(23) = 4.10379 |
K(24)
= 4.38277 |
C(24)
= 4.44077 |
K(25)
= 4.76361 |
C(25) = 4.61570 |
K(26)
- K(29) |
|
= 5.000000 |
|
Figure
8.4. The fractional deviation of values of the adopted database from the
recommended values for the entropy integrated from the heat capacity spline.
Table 8.5. Recommended values
of entropy of liquid 4He obtained by integration of the heat capacity
spline.
T90 (K) |
S (J/g K) |
T90 (K) |
S
(J/g K) |
0.10 |
6.600E-6 |
2.25
|
1.720E+0 |
0.15 |
2.298E-5 |
2.30
|
1.783E+0 |
0.20
|
5.506E-5
|
2.35
|
1.838E+0 |
0.25
|
1.074E-4
|
2.40
|
1.890E+0 |
0.30 |
1.841E-4 |
2.45 |
1.939E+0 |
0.35 |
2.898E-4 |
2.50 |
1.985E+0 |
0.40
|
4.298E-4
|
2.55
|
2.030E+0 |
0.45
|
6.093E-4
|
2.60
|
2.074E+0 |
0.50
|
8.343E-4
|
2.65
|
2.116E+0 |
0.55
|
1.113E-3
|
2.70
|
2.158E+0 |
0.60
|
1.456E-3
|
2.75 |
2.200E+0 |
0.65
|
1.904E-3 |
2.80 |
2.242E+0 |
0.70
|
2.512E-3
|
2.85 |
2.284E+0 |
0.75
|
3.339E-3
|
2.90 |
2.326E+0 |
0.80
|
4.512E-3
|
2.95 |
2.367E+0 |
0.85
|
6.206E-3
|
3.00 |
2.409E+0 |
0.90 |
8.605E-3 |
3.05
|
2.451E+0 |
0.95
|
1.194E-2
|
3.10 |
2.492E+0 |
1.00
|
1.644E-2 |
3.15 |
2.534E+0 |
1.05
|
2.236E-2
|
3.20 |
2.576E+0 |
1.10
|
3.004E-2
|
3.25
|
2.619E+0 |
1.15
|
3.982E-2
|
3.30
|
2.661E+0 |
1.20 |
5.204E-2 |
3.35 |
2.704E+0 |
1.25 |
6.706E-2 |
3.40 |
2.747E+0 |
1.30
|
8.521E-2
|
3.45
|
2.790E+0 |
1.35
|
1.068E-1
|
3.50
|
2.834E+0 |
1.40
|
1.323E-1 |
3.55
|
2.878E+0 |
1.45
|
1.620E-1 |
3.60 |
2.923E+0 |
1.50
|
1.965E-1
|
3.70
|
3.014E+0 |
1.55
|
2.364E-1
|
3.75
|
3.060E+0 |
1.60 |
2.824E-1 |
3.80 |
3.107E+0 |
1.65
|
3.350E-1
|
3.85
|
3.154E+0 |
1.70
|
3.950E-1
|
3.90 |
3.203E+0 |
1.75
|
4.630E-1
|
3.95 |
3.251E+0 |
1.80
|
5.399E-1
|
4.00
|
3.301E+0 |
1.85
|
6.270E-1
|
4.05
|
3.351E+0 |
1.90
|
7.255E-1
|
4.10
|
3.402E+0 |
1.95
|
8.367E-1
|
4.15 |
3.454E+0 |
2.00
|
9.621E-1
|
4.20 |
3.507E+0 |
2.05
|
1.103E+0
|
4.25 |
3.561E+0 |
2.10
|
1.263E+0
|
4.30 |
3.616E+0 |
2.1760
|
1.578E+0
|
4.35
|
3.672E+0 |
2.1762 |
1.579E+0 |
4.40
|
3.728E+0 |
2.1763
|
1.580E+0
|
4.45
|
3.786E+0 |
2.1764
|
1.580E+0
|
4.50
|
3.846E+0 |
2.1765 |
1.581E+0 |
4.75
|
4.175E+0 |
2.1766
|
1.581E+0
|
4.80 |
4.250E+0 |
2.1767
|
1.582E+0
|
4.85 |
4.330E+0 |
2.1768
|
1.583E+0
|
4.90
|
4.416E+0 |
2.1769 |
1.583E+0 |
4.95 |
4.511E+0 |
2.1770
|
1.583E+0
|
5.00 |
4.616E+0 |
2.20 |
1.643E+0 |
|
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Chronological Bibliography for Entropy
1 |
H. C. Kramers, J. D. Wasscher, and C. J. Gorter, "The Specific Heat
of Liquid Helium Between 0.25 and 1.9 Degrees K," Physica 18, 329-337
(1952). |
2 |
G.
R. Hercus and J. Wilks, “The Specific Heat of Liquid Helium
II as a Function of Pressure,” Philos. Mag. 45, 1163-1172 (1954). |
3 |
O.
V. Lounasmaa and E. Kojo, “The Specific Heat Cv of Liquid Helium
Near the Lambda Curve at Various Densities,” Ann. Acad. Scien.
Fennicae A VI, Physica 36, 1 (1959). |
4 |
C.
J. N. Van den Meijdenberg, K. W. Taconis, and R. De Bruyn Ouboter,
“The Entropy of Helium II Under Pressure from Measurements on
the Fountain Effect,” Physica 27, 197-218 (1961). |
5 |
J.
Wiebes, “Caloric Measurements on Liquid and Melting Helium Below
1.5 Kelvin,” Ph.D. Thesis, Kammerlingh Onnes Laboratory, 1969
(unpublished). |
6 |
A.
L. Singsaas and G. Ahlers, “Entropy of Helium II from 1.6 K
to the Lambda Line,” Phys. Rev. B 29, 4951-4960 (1983). |
7 |
A.
L. Singsaas, “Entropy of Helium II and Universality Near the
Superfluid Transition in 4He,” Ph.D. Thesis, University of California,
1984 (unpublished) |
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