|
|
The
Observed Properties of Liquid Helium
at the Saturated Vapor
Pressure
Chapter 7. Heat Capacity and Enthalpy
Adopted
Database
Author(s) |
Key # |
Method |
Range (K) |
Uncertainty % |
Donnelly |
1 |
Theory |
0.01
T
0.06 |
NA |
Greywall |
2 |
Calorimeter |
0.0606
T
1.024 |
1 |
Wiebes |
3 |
Calorimeter |
0.3
T
1.6 |
2 |
Phillips |
4 |
Calorimeter |
0.32161
T
2.17805 |
1 |
Buckingham |
5 |
Calorimeter |
2.072
T
2.272 |
3 |
Ahlers |
6 |
Calorimeter |
2.17282
T
2.17805 |
1 |
Lipa |
7 |
Calorimeter |
2.1699103
T
2.1740277 |
1.5 |
Hill |
8 |
Calorimeter |
2.1992
T 5.50543
|
1 |
Comments
and Key to Authors
1)
Ref. 14. Calculated from the Landau theory.
2) Ref. 15 and 16. Temperatures taken on 1962 3He Scale.
3) Ref. 9.
4) Ref. 10.
5) Ref. 6, page 85.
6) Ref. 11.
7) Ref. 17. Temperatures taken on the EPT-76 scale.
8) Ref. 3. Corrected to T58.
9) The spline is actually fit to , where Cs is the heat capacity
at saturation pressure.
10) Lipa et. al. Ref. 16 have measured Cs very near the lambda
point in a microgravity experiment. They fit their data using functions
of the type , where t=|
1+ T/T
|. was set at 0.5 above and below T.
The results were as follows:
The range of data for T
T
was , and for T
T
was . The data above T
are not considered as accurate as the data below T.
11) The enthalpy H of liquid helium can be deduced from the heat capacity
using the relation
where
the second term arises because we are following along the saturated vapor
pressure line. H is the difference between the total enthalpy and the
ground state enthalpy (see J. S. Brooks and R. J. Donnelly, J. Phys. Chem.
Ref. Data p. 51 1977, Section 4.3.d).
Figure
7.1. The recommended values for the heat capacity of liquid 4He as a function
of temperature at saturated vapor pressure.
12) We list recommended values of enthalpy directly from the above integration,
so the uncertainties reflect uncertainties in heat capacity. We have also
given a spline of the enthalpy for convenience of the reader. The spline
does not return the exact recommended values (see Fig. 7.7).
13) Most heat capacity measurements are reported in Joules/mol•K.
To convert data from J/g•K to J/mol•K multiply by 4.0026.
To convert from Joules/mol•K to J/kg•K multiply by 249.837.
The same factor is used to convert the units for enthalpy.
Figure
7.2. The recommended values for the heat capacity of liquid 4He at saturated
vapor pressure near expressed as vs Log10|T-T|.
Figure
7.3. The fractional deviation of values of the adopted database from the
recommended values for the heat capacity of liquid 4He expressed in percent.
Figure
7.4. The fractional deviation of values of the adopted database from the
recommended values for the heat capacity of liquid 4He near the lambda
transition for T < T.
Figure
7.5. The fractional deviation of values of the adopted database from the
recommended values for the heat capacity of liquid 4He near the lambda
transition for T > T.
Figure
7.6. Values for the enthalpy of liquid 4He at saturated vapor pressure,
obtained by integration of the recommended values of the heat capacity.
Figure 7.7. Fractional deviation
of the spline fit of the recommended values of the enthalpy from the enthalpy
integrated from recommended values of the heat capacity.
Table 7.1. Adopted database
for heat capacity of liquid 4He at saturated vapor
T90 (K) |
Cs (J/mol·K) |
Key |
T90 |
u1 (m/s) |
Key |
0.010000000
|
8.31700E-08
|
1
|
0.332900000
|
2.95200E-03 |
2 |
0.015000000
|
2.80670E-07
|
1
|
0.337236048
|
3.05200E-03
|
4 |
0.020075015
|
6.65200E-07
|
1 |
0.339201980
|
3.16100E-03 |
4 |
0.025093607
|
1.29900E-06 |
1 |
0.349400000
|
3.39700E-03 |
2 |
0.030112134
|
2.24456E-06 |
1 |
0.351177931
|
3.48226E-03 |
3 |
0.035130597
|
3.56360E-06 |
1 |
0.353755696 |
3.58300E-03 |
4 |
0.040148997
|
5.31800E-06
|
1
|
0.358810557
|
3.73000E-03 |
4 |
0.045167333
|
7.57050E-06 |
1 |
0.366700000
|
3.90200E-03 |
2 |
0.050185606
|
1.03800E-05
|
1 |
0.371879445
|
4.13900E-03 |
4 |
0.055203817
|
1.38140E-05 |
1
|
0.380223962 |
4.40300E-03
|
4 |
0.060221963
|
1.79290E-05
|
1 |
0.384700000 |
4.48700E-03
|
2 |
0.060610000
|
1.70500E-05 |
2 |
0.391476993
|
4.79500E-03 |
4 |
0.063540000
|
1.97600E-05 |
2 |
0.401325554
|
5.24341E-03 |
3 |
0.066640000
|
2.31700E-05
|
2 |
0.401800000
|
5.09000E-03
|
2 |
0.069870000
|
2.71300E-05 |
2 |
0.403451755
|
5.25600E-03 |
4 |
0.073270000
|
3.16800E-05
|
2 |
0.412929109 |
5.59100E-03
|
4 |
0.076860000
|
3.67400E-05
|
2
|
0.417900000
|
5.71000E-03 |
2 |
0.080670000
|
4.28200E-05
|
2
|
0.428112594
|
6.23700E-03 |
4 |
0.084630000
|
4.96100E-05
|
2 |
0.433600000
|
6.36400E-03
|
2 |
0.088820000
|
5.73600E-05
|
2
|
0.436847534
|
6.59600E-03
|
4 |
0.093220000
|
6.66700E-05 |
2 |
0.448800000
|
7.03900E-03
|
2 |
0.097810000
|
7.70700E-05 |
2
|
0.451468481
|
7.44484E-03 |
3 |
0.102800000
|
8.99000E-05
|
2 |
0.454136258 |
7.44200E-03
|
4 |
0.108000000
|
1.04600E-04
|
2
|
0.463700000 |
7.75900E-03 |
2 |
0.113500000
|
1.21200E-04
|
2
|
0.464605602
|
7.94600E-03 |
4 |
0.119400000
|
1.41500E-04 |
2 |
0.478200000
|
8.51600E-03
|
2 |
0.125500000
|
1.64800E-04
|
2 |
0.483407690
|
8.97200E-03
|
4 |
0.132000000
|
1.91000E-04 |
2
|
0.492800000
|
9.34200E-03 |
2 |
0.138800000
|
2.22500E-04
|
2
|
0.497085329
|
9.78200E-03
|
4 |
0.146200000
|
2.60500E-04 |
2
|
0.501607656
|
1.02867E-02 |
3 |
0.153900000
|
3.02900E-04 |
2 |
0.507100000
|
1.02100E-02
|
2 |
0.161900000
|
3.52700E-04
|
2
|
0.514462524
|
1.08900E-02
|
4 |
0.170200000
|
4.09200E-04 |
2 |
0.521500000
|
1.11700E-02 |
2 |
0.179200000
|
4.77200E-04 |
2
|
0.523617428
|
1.15100E-02 |
4 |
0.188800000
|
5.56700E-04
|
2 |
0.535900000
|
1.22200E-02
|
2 |
0.198800000
|
6.49000E-04
|
2
|
0.546077483
|
1.32000E-02 |
4 |
0.209500000
|
7.56800E-04
|
2
|
0.550700000
|
1.34205E-02
|
2 |
0.220600000
|
8.82600E-04
|
2
|
0.551742562
|
1.40491E-02 |
3 |
0.231700000
|
1.01900E-03 |
2 |
0.555683078
|
1.40300E-02 |
4 |
0.244100000
|
1.18900E-03 |
2 |
0.565687962
|
1.47675E-02 |
2 |
0.257300000
|
1.38900E-03 |
2 |
0.576517791 |
1.60300E-02
|
4 |
0.272200000
|
1.64100E-03
|
2
|
0.580874318
|
1.62819E-02 |
2 |
0.286700000
|
1.90900E-03
|
2
|
0.588478962
|
1.73300E-02
|
4 |
0.301025619
|
2.20143E-03
|
3
|
0.596225336
|
1.80215E-02
|
2 |
0.301900000
|
2.22300E-03
|
2
|
0.601873568
|
1.94927E-02
|
3 |
0.317100000
|
2.57000E-03
|
2 |
0.612103323 |
2.00869E-02 |
2 |
0.322702023
|
2.69800E-03
|
4 |
0.612310364
|
2.04600E-02 |
4 |
Table
7.1. (Continued)
T90 (K) |
Cs (J/mol·K) |
Key |
T90 |
u1 (m/s) |
Key |
0.626807284
|
2.26300E-02
|
4
|
1.388218288
|
3.01900E+00 |
4 |
0.628517095
|
2.25628E-02
|
2 |
1.403515049
|
3.09001E+00 |
3 |
0.645456333
|
2.55163E-02
|
2 |
1.453556614
|
3.72642E+00 |
3 |
0.648852852
|
2.65700E-02
|
4
|
1.503597910
|
4.46290E+00
|
3 |
0.651991318
|
2.78981E-02 |
3 |
1.505409334
|
4.58000E+00 |
4 |
0.662934853
|
2.90934E-02 |
2 |
1.505899719
|
4.68500E+00 |
4 |
0.681197115
|
3.34762E-02 |
2 |
1.553637123
|
5.32346E+00
|
3 |
0.691277949
|
3.70400E-02 |
4 |
1.582153782
|
5.90600E+00
|
4 |
0.700368882
|
3.90665E-02
|
2 |
1.603690373 |
6.31610E+00 |
3 |
0.702124626
|
4.11868E-02
|
3
|
1.635233195
|
7.20800E+00 |
4 |
0.708499999
|
4.25700E-02
|
4
|
1.658829565
|
7.56400E+00 |
4 |
0.720452604
|
4.59791E-02
|
2 |
1.754802154
|
1.02300E+01 |
4 |
0.741502751
|
5.47328E-02
|
2 |
1.776611822
|
1.10800E+01 |
4 |
0.750478191
|
6.05000E-02 |
4 |
1.865627080
|
1.43200E+01 |
4 |
0.752244790
|
6.18402E-02
|
3 |
1.916469079
|
1.65500E+01 |
4 |
0.763992981
|
6.60381E-02
|
2
|
1.992102080
|
2.08800E+01
|
4 |
0.766438104
|
6.88300E-02
|
4
|
1.996426104
|
2.07500E+01
|
4 |
0.787875344
|
8.05773E-02
|
2 |
2.052220307
|
2.47400E+01
|
4 |
0.802361834
|
9.28603E-02
|
3
|
2.062756913
|
2.56400E+01
|
4 |
0.814481920
|
1.00959E-01
|
2
|
2.063718535
|
2.56800E+01
|
4 |
0.815742366
|
1.03700E-01
|
4 |
2.065000728 |
2.58100E+01
|
4 |
0.836419447
|
1.23600E-01 |
4 |
2.066713713
|
2.59400E+01
|
4 |
0.841734070
|
1.26561E-01
|
2
|
2.068767375
|
2.61400E+01
|
4 |
0.852475684
|
1.38890E-01
|
3
|
2.070811114
|
2.63000E+01
|
4 |
0.871304640
|
1.60808E-01
|
2 |
2.076331708
|
2.63771E+01
|
5 |
0.877089828
|
1.68900E-01 |
4 |
2.113325831
|
3.06599E+01
|
5 |
0.902586267
|
2.05734E-01
|
3 |
2.123709861
|
3.26700E+01
|
4 |
0.903629130
|
2.07131E-01 |
2 |
2.136704232 |
3.36619E+01 |
5 |
0.906374498
|
2.11000E-01
|
4 |
2.140798148
|
3.40400E+01
|
6 |
0.939237630
|
2.70084E-01
|
2
|
2.144510586
|
3.49400E+01 |
6 |
0.943765008
|
2.78600E-01
|
4
|
2.148814681
|
3.58900E+01 |
6 |
0.952694176
|
2.98594E-01
|
3 |
2.151453098
|
3.68239E+01
|
5 |
0.975031504
|
3.47300E-01
|
4 |
2.159768125
|
3.91700E+01 |
6 |
0.978888050
|
3.57773E-01
|
2 |
2.160680705
|
3.95857E+01
|
5 |
1.002776612
|
4.23075E-01
|
3 |
2.160690733 |
3.94800E+01 |
6 |
1.012518339 |
4.46700E-01 |
4 |
2.162395451 |
3.97600E+01 |
6 |
1.023530400
|
4.81150E-01
|
2 |
2.165754329 |
4.17600E+01
|
6 |
1.052861275
|
5.83579E-01 |
3 |
2.166596462
|
4.23000E+01
|
6 |
1.088881255
|
7.17000E-01
|
4 |
2.166596462
|
4.22274E+01 |
5 |
1.102955222
|
7.84109E-01
|
3 |
2.167318259 |
4.30600E+01
|
4 |
1.153029266
|
1.02867E+00
|
3 |
2.167439558
|
4.27600E+01 |
6 |
1.172802215
|
1.14300E+00 |
4 |
2.168030001
|
4.33000E+01
|
4 |
1.203266846
|
1.32086E+00
|
3
|
2.168932168
|
4.40900E+01 |
4 |
1.253202675
|
1.66508E+00 |
3 |
2.169107584
|
4.38900E+01
|
6 |
1.277869986
|
1.91000E+00 |
4
|
2.169543609
|
4.45600E+01 |
4 |
1.303323993
|
2.06934E+00
|
3
|
2.169944542
|
4.46000E+01 |
6 |
1.353442881
|
2.54165E+00
|
3
|
2.170072838
|
4.46700E+01 |
6 |
Table
7.1. (Continued)
T90 (K) |
Cs (J/mol·K) |
Key |
T90 |
u1 (m/s) |
Key |
2.170305372
|
4.48691E+01
|
5
|
2.175579900
|
5.35000E+01 |
7 |
2.170405602
|
4.55200E+01 |
4
|
2.175647000
|
5.40200E+01 |
6 |
2.170406604
|
4.49200E+01
|
6 |
2.175670300
|
5.40000E+01 |
7 |
2.170744372
|
4.52500E+01
|
6
|
2.175717000
|
5.42800E+01 |
6 |
2.170936807
|
4.61800E+01
|
4
|
2.175745000
|
5.44400E+01
|
6 |
2.171087144
|
4.55400E+01
|
6 |
2.175760500
|
5.43000E+01
|
7 |
2.171287593
|
4.58100E+01 |
4 |
2.175792000
|
5.46000E+01 |
6 |
2.171438929
|
4.59300E+01
|
6
|
2.175800000
|
5.45554E+01 |
5 |
2.171528127
|
4.67700E+01 |
4 |
2.175831310
|
5.48000E+01
|
7 |
2.171973000
|
4.62700E+01 |
6 |
2.175899950 |
5.52000E+01 |
7 |
2.172030000
|
4.70500E+01 |
4 |
2.175911900
|
5.52200E+01 |
6 |
2.172151000
|
4.65200E+01
|
6 |
2.175960800
|
5.55600E+01 |
6 |
2.172320000
|
4.82000E+01 |
4 |
2.175970830
|
5.56000E+01 |
7 |
2.172428000
|
4.68600E+01 |
6
|
2.176002800
|
5.59200E+01
|
6 |
2.172645000
|
4.70700E+01
|
6 |
2.176029750 |
5.59000E+01
|
7 |
2.172820000
|
4.71106E+01
|
5 |
2.176050500 |
5.62000E+01
|
6 |
2.172830000
|
4.82900E+01 |
4 |
2.176080300
|
5.63600E+01 |
6 |
2.172983000
|
4.76000E+01 |
6 |
2.176090610 |
5.62000E+01
|
7 |
2.173111000
|
4.77900E+01
|
6
|
2.176129200
|
5.67200E+01 |
6 |
2.173322000
|
4.80600E+01 |
6 |
2.176141490
|
5.67000E+01
|
7 |
2.173664000
|
4.86100E+01
|
6 |
2.176175600
|
5.70300E+01
|
6 |
2.173710000
|
4.97300E+01 |
4 |
2.176180490
|
5.69000E+01 |
7 |
2.173767000
|
4.88600E+01
|
6 |
2.176230510 |
5.76000E+01 |
7 |
2.174008000
|
4.92300E+01
|
6 |
2.176281960
|
5.79000E+01
|
7 |
2.174173000
|
4.96100E+01 |
6
|
2.176282500
|
5.79700E+01 |
6 |
2.174290000
|
4.97123E+01
|
5
|
2.176297000
|
5.83000E+01
|
6 |
2.174340000
|
4.98800E+01
|
6 |
2.176300000
|
5.75974E+01 |
5 |
2.174673000 |
5.06500E+01 |
6 |
2.176302700 |
5.83200E+01 |
6 |
2.174710300 |
5.06000E+01 |
7 |
2.176313500 |
5.83400E+01 |
6 |
2.174843000 |
5.11200E+01 |
6 |
2.176319470 |
5.83000E+01 |
7 |
2.174860600 |
5.12000E+01 |
7 |
2.176326100 |
5.84600E+01 |
6 |
2.175044000 |
5.17100E+01 |
6 |
2.176351800 |
5.89800E+01 |
6 |
2.175075000 |
5.17900E+01 |
6 |
2.176380650 |
5.91000E+01 |
7 |
2.175079000 |
5.18400E+01 |
6 |
2.176410970 |
5.95000E+01 |
7 |
2.175140500 |
5.21000E+01 |
7 |
2.176441060 |
5.99000E+01 |
7 |
2.175210000 |
5.23540E+01 |
5 |
2.176446700 |
6.00400E+01 |
6 |
2.175244000 |
5.22800E+01 |
6 |
2.176465200 |
6.03100E+01 |
6 |
2.175261600 |
5.24000E+01 |
7 |
2.176471930 |
6.02000E+01 |
7 |
2.175318000 |
5.26000E+01 |
6 |
2.176482200 |
6.05000E+01 |
6 |
2.175370300 |
5.26000E+01 |
7 |
2.176489950 |
6.04000E+01 |
7 |
2.175383000 |
5.28500E+01 |
6 |
2.176511500 |
6.10500E+01 |
6 |
2.175411000 |
5.29300E+01 |
6 |
2.176517430 |
6.11000E+01 |
7 |
2.175480300 |
5.31000E+01 |
7 |
2.176537170 |
6.14000E+01 |
7 |
2.175514000 |
5.33200E+01 |
6 |
2.176556820 |
6.18000E+01 |
7 |
2.175578000 |
5.35800E+01 |
6 |
2.176572560 |
6.20000E+01 |
7 |
T90 (K) |
Cs (J/mol·K) |
Key |
T90 |
u1 (m/s) |
Key |
2.176583200 |
6.24000E+01 |
6 |
2.176783965 |
7.57000E+01 |
7 |
2.176589940
| 6.27000E+01 |
7 |
2.176784972 |
7.60000E+01 |
7 |
2.176600000 |
6.12398E+01 |
5 |
2.176785500 |
7.60000E+01 |
6 |
2.176606060 |
6.32000E+01 |
7 |
2.176785700 |
7.71000E+01 |
6 |
2.176615000 |
6.32900E+01 |
6 |
2.176786010 |
7.61000E+01 |
7 |
2.176619900 |
6.37000E+01 |
6 |
2.176787021 |
7.65000E+01 |
7 |
2.176620470 |
6.32000E+01 |
7 |
2.176787994 |
7.69000E+01 |
7 |
2.176631500 |
6.38800E+01 |
6 |
2.176788956 |
7.73000E+01 |
7 |
2.176636230 |
6.37000E+01 |
7 |
2.176789967 |
7.76000E+01 |
7 |
2.176645370 |
6.40000E+01 |
7 |
2.176790000 |
7.77000E+01 |
6 |
2.176655790 |
6.46000E+01 |
7 |
2.176790000 |
7.76504E+01 |
5 |
2.176665910 |
6.46000E+01 |
7 |
2.176790200 |
7.80000E+01 |
6 |
2.176671800 |
6.52800E+01 |
6 |
2.176790792 |
7.77000E+01 |
7 |
2.176675720 |
6.53000E+01 |
7 |
2.176791479 |
7.87000E+01 |
7 |
2.176678000 |
6.55100E+01 |
6 |
2.176792234 |
7.88000E+01 |
7 |
2.176678500 |
6.53700E+01 |
6 |
2.176792744 |
7.87000E+01 |
7 |
2.176685000 |
6.57000E+01 |
7 |
2.176793259 |
8.02000E+01 |
7 |
2.176695450 |
6.59000E+01 |
7 |
2.176793869 |
8.05000E+01 |
7 |
2.176700000 |
6.60829E+01 |
5 |
2.176794309 |
8.04000E+01 |
7 |
2.176704242 |
6.65000E+01 |
7 |
2.176794761 |
8.10000E+01 |
7 |
2.176710628 |
6.70000E+01 |
7 |
2.176795229 |
8.13000E+01 |
7 |
2.176716977 |
6.73000E+01 |
7 |
2.176795659 |
8.16000E+01 |
7 |
2.176723343 |
6.78000E+01 |
7 |
2.176795979 |
8.21000E+01 |
7 |
2.176728740 |
6.76000E+01 |
7 |
2.176796282 |
8.23000E+01 |
7 |
2.176734305 |
6.85000E+01 |
7 |
2.176796663 |
8.29000E+01 |
7 |
2.176738974 |
6.92000E+01 |
7 |
2.176796931 |
8.42000E+01 |
7 |
2.176744134 |
6.90000E+01 |
7 |
2.176797220 |
8.38000E+01 |
7 |
2.176748459 |
6.95000E+01 |
7 |
2.176797379 |
8.41000E+01 |
7 |
2.176750000 |
6.96452E+01 |
5 |
2.176797628 |
8.47000E+01 |
7 |
2.176751982 |
7.02000E+01 |
7 |
2.176797839 |
8.56000E+01 |
7 |
2.176755459 |
7.03000E+01 |
7 |
2.176798079 |
8.56000E+01 |
7 |
2.176758801 |
7.06000E+01 |
7 |
2.176798200 |
8.58000E+01 |
7 |
2.176762052 |
7.12000E+01 |
7 |
2.176798379 |
8.64000E+01 |
7 |
2.176764908 |
7.15000E+01 |
7 |
2.176798527 |
8.79000E+01 |
7 |
2.176767701 |
7.18000E+01 |
7 |
2.176798835 |
8.88000E+01 |
7 |
2.176769257 |
7.13000E+01 |
7 |
2.176798931 |
8.86000E+01 |
7 |
2.176771289 |
7.26000E+01 |
7 |
2.176799028 |
8.87000E+01 |
7 |
2.176773790 |
7.27000E+01 |
7 |
2.176799128 |
8.93000E+01 |
7 |
2.176775441 |
7.34000E+01 |
7 |
2.176799229 |
8.99000E+01 |
7 |
2.176777369 |
7.36000E+01 |
7 |
2.176799328 |
9.05000E+01 |
7 |
2.176779885 |
7.44000E+01 |
7 |
2.176799429 |
9.14000E+01 |
7 |
2.176780000 |
7.38480E+01 |
5 |
2.176799523 |
9.26000E+01 |
7 |
2.176780922 |
7.47000E+01 |
7 |
2.176799584 |
9.24000E+01 |
7 |
2.176781000 |
7.40000E+01 |
6 |
2.176799650 |
9.28000E+01 |
7 |
2.176781600 |
7.59000E+01 |
6 |
2.176799725 |
9.47000E+01 |
7 |
2.176782511 |
7.51000E+01 |
7 |
2.176799768 |
9.59000E+01 |
7 |
Table
7.1. (Continued)
T90 (K) |
Cs (J/mol·K) |
Key |
T90 |
u1 (m/s) |
Key |
2.176799822 |
9.65000E+01 |
7
|
2.176807642 |
5.95000E+01 |
7 |
2.176799860 |
9.72000E+01 |
7 |
2.176808443 |
5.92000E+01 |
7 |
2.176799909 |
1.00000E+02 |
7 |
2.176809033 |
5.85000E+01 |
7 |
2.176799965 |
1.04100E+02 |
7 |
2.176809600 |
5.68000E+01 |
6 |
2.176800132 |
7.95000E+01 |
7 |
2.176809698 |
5.81000E+01 |
7 |
2.176800144 |
7.97000E+01 |
7 |
2.176810000 |
5.76000E+01 |
6 |
2.176800164 |
7.99000E+01 |
7 |
2.176810000 |
5.76374E+01 |
5 |
2.176800185 |
7.95000E+01 |
7 |
2.176810569 |
5.78000E+01 |
7 |
2.176800220 |
7.89000E+01 |
7 |
2.176811400 |
5.71000E+01 |
6 |
2.176800269 |
7.67000E+01 |
7 |
2.176811505 |
5.71000E+01 |
7 |
2.176800293 |
7.60000E+01 |
7 |
2.176812520 |
5.69000E+01 |
7 |
2.176800320 |
7.68000E+01 |
7 |
2.176813463 |
5.63000E+01 |
7 |
2.176800371 |
7.56000E+01 |
7 |
2.176814493 |
5.64000E+01 |
7 |
2.176800400 |
7.36000E+01 |
7 |
2.176815612 |
5.58000E+01 |
7 |
2.176800420 |
7.33000E+01 |
7 |
2.176816537 |
5.52000E+01 |
7 |
2.176800494 |
7.35000E+01 |
7 |
2.176816800 |
5.37000E+0 |
6 |
2.176800593 |
7.24000E+01 |
7 |
2.176817900 |
5.46000E+01 |
6 |
2.176800692 |
7.15000E+01 |
7 |
2.176818091 |
5.48000E+01 |
7 |
2.176800797 |
7.07000E+01 |
7 |
2.176819577 |
5.45000E+01 |
7 |
2.176800896 |
7.04000E+01 |
7 |
2.176820000 |
5.46355E+01 |
5 |
2.176800998 |
6.99000E+01 |
7 |
2.176821081 |
5.42000E+01 |
7 |
2.176801097 |
6.95000E+01 |
7 |
2.176823067 |
5.35000E+01 |
7 |
2.176801171 |
6.88000E+01 |
7 |
2.176825087 |
5.35000E+01 |
7 |
2.176801296 |
6.83000E+01 |
7 |
2.176827095 |
5.30000E+01 |
7 |
2.176801363 |
6.84000E+01 |
7 |
2.176829050 |
5.26000E+01 |
7 |
2.176801494 |
6.76000E+01 |
7 |
2.176831035 |
5.25000E+01 |
7 |
2.176801568 |
6.79000E+01 |
7 |
2.176832778 |
5.18000E+01 |
7 |
2.176801724 |
6.81000E+01 |
7 |
2.176835750 |
5.12000E+01 |
7 |
2.176801849 |
6.62000E+01 |
7 |
2.176837100 |
5.10000E+01 |
6 |
2.176801969 |
6.64000E+01 |
7 |
2.176838888 |
5.06000E+01 |
7 |
2.176802149 |
6.66000E+01 |
7 |
2.176841885 |
5.05000E+01 |
7 |
2.176802342 |
6.58000E+01 |
7 |
2.176844784 |
5.00000E+01 |
7 |
2.176802516 |
6.52000E+01 |
7 |
2.176848510 |
4.98000E+01 |
7 |
2.176802675 |
6.44000E+01 |
7 |
2.176850000 |
4.96322E+01 |
5 |
2.176802906 |
6.40000E+01 |
7 |
2.176852300 |
4.93000E+01 |
6 |
2.176803147 |
6.37000E+01 |
7 |
2.176852561 |
4.92000E+01 |
7 |
2.176803331 |
6.35000E+01 |
7 |
2.176856247 |
4.90000E+01 |
7 |
2.176803593 |
6.31000E+01 |
7 |
2.176861043 |
4.88000E+01 |
7 |
2.176803900 |
6.28000E+01 |
7 |
2.176866602 |
4.78000E+01 |
7 |
2.176804196 |
6.25000E+01 |
7 |
2.176871084 |
4.77000E+01 |
7 |
2.176804544 |
6.18000E+01 |
7 |
2.176872600 |
4.73000E+01 |
6 |
2.176804944 |
6.14000E+01 |
7 |
2.176876677 |
4.74000E+01 |
7 |
2.176805319 |
6.13000E+01 |
7 |
2.176882637 |
4.68000E+01 |
7 |
2.176805743 |
6.08000E+01 |
7 |
2.176888300 |
4.64000E+01 |
6 |
2.176806207 |
6.02000E+01 |
7 |
2.176888888 |
4.68000E+01 |
7 |
2.176806697 |
6.00000E+01 |
7 |
2.176889500 |
4.61400E+01 |
6 |
2.176807203 |
5.95000E+01 |
7 |
.176897038 |
4.63000E+01 |
7 |
Table
7.1. (Continued)
T90 (K) |
Cs (J/mol·K) |
Key |
T90 |
u1 (m/s) |
Key |
2.176900000 |
4.52694E+01 |
5 |
2.178240900 |
3.15000E+01 |
7 |
2.176905090 |
4.56000E+01 |
7 |
2.178341000 |
3.12000E+01 |
7 |
2.176915210 |
4.50000E+01 |
7 |
2.178390000 |
3.11803E+01 |
5 |
2.176924970 |
4.47000E+01 |
7 |
2.178450300 |
3.09000E+01 |
7 |
2.176934900 |
4.45000E+01 |
7 |
2.178524000 |
3.04300E+01 |
6 |
2.176945050 |
4.36000E+01 |
7 |
2.178590400 |
3.03000E+01 |
7 |
2.176955460 |
4.36000E+01 |
7 |
2.178678000 |
2.99900E+01 |
6 |
2.176964320 |
4.31000E+01 |
7 |
2.178740200 |
3.00000E+01 |
7 |
2.176972800 |
4.27500E+01 |
6 |
2.178827700 |
2.99000E+01 |
7 |
2.176979650 |
4.27000E+01 |
7 |
2.178869000 |
600E+01 |
6 |
2.176995040 |
4.19000E+01 |
7 |
2.179214000 |
2.86400E+01 |
6 |
2.177000000 |
4.23075E+01 |
5 |
2.179310000 |
2.87387E+01 |
5 |
2.177010690 |
4.19000E+01 |
7 |
2.179553000 |
2.79300E+01 |
6 |
2.177028050 |
4.14000E+01 |
7 |
2.179814000 |
2.74800E+01 |
6 |
2.177037900 |
4.10800E+01 |
6 |
2.179880000 |
2.73300E+01 |
6 |
2.177043600 |
4.11000E+01 |
7 |
2.180204000 |
2.68000E+01 |
6 |
2.177065760 |
4.06000E+01 |
7 |
2.180749000 |
2.60400E+01 |
6 |
2.177066000 |
4.04300E+01 |
6 |
2.180780000 |
2.65372E+01 |
5 |
2.177087900 |
4.04000E+01 |
7 |
2.181431000 |
2.52000E+01 |
6 |
2.177109540 |
3.99000E+01 |
7 |
2.181963955 |
2.44400E+01 |
6 |
2.177129670 |
3.95000E+01 |
7 |
2.182673184 |
2.37700E+01 |
6 |
2.177159490 |
3.90000E+01 |
7 |
2.182925239 |
2.36954E+01 |
5 |
2.177189620 |
3
.85000E+01 |
7 |
2.186624998 |
2.12138E+01 |
5 |
2.177219030
|
3.84000E+01 |
7 |
2.192523901 |
1.87722E+01 |
5 |
2.177238300 |
3.77800E+01 |
6 |
2.201723640 |
1.65708E+01 |
5 |
2.177250520 |
3.80000E+01 |
7 |
2.203823802 |
1.59304E+01 |
8 |
2.177282540 |
3.71000E+01 |
7 |
2.216426239 |
1.46535E+01 |
5 |
2.177300000 |
3.68239E+01 |
5 |
2.23973624 |
1.28363E+01 |
5 |
2.177309700 |
3.69800E+01 |
6 |
2.25384544 |
1.21679E+01 |
8 |
2.177319440 |
3.70000E+01 |
7 |
2.276666284 |
1.14194E+01 |
5 |
2.177369760 |
3.65000E+01 |
7 |
2.304205527 |
1.05669E+01 |
8 |
2.177421430 |
3.60000E+01 |
7 |
2.354513418 |
9.88647E+00 |
8 |
2.177461300 |
3.58000E+01 |
7 |
2.404936229 |
9.52620E+00 |
8 |
2.177485500 |
3.54100E+01 |
6 |
2.505557267 |
9.12590E+00 |
8 |
2.177510100 |
3.53000E+01 |
7 |
2.606086904 |
9.08590E+00 |
8 |
2.177570830 |
3.48000E+01 |
7 |
2.706596360 |
9.16590E+00 |
8 |
2.177628930 |
3.45000E+01 |
7 |
2.807058930 |
9.36610E+00 |
8 |
2.177700280 |
3.40000E+01 |
7 |
2.907241720 |
9.64630E+00 |
8 |
2.177771260 |
3.37000E+01 |
7 |
3.007401739 |
9.96650E+00 |
8 |
2.177800000 |
3.34617E+01 |
5 |
.107543262 |
1.03267E+01 |
8 |
2.177825000 |
3.32200E+01 |
6 |
3.207478906 |
1.07670E+01 |
8 |
2.177850200 |
3.32000E+01 |
7 |
3.307424279 |
1.13274E+01 |
8 |
2.177938900 |
3.28000E+01 |
7 |
3.407351902 |
1.18877E+01 |
8 |
2.177984000 |
3.25000E+01 |
6 |
3.507252795 |
1.24481E+01 |
8 |
2.178029200 |
3.24000E+01 |
7 |
3.607129693 |
1.30485E+01 |
8 |
2.178129400 |
3.20000E+01 |
7 |
3.707066600 |
1.36889E+01 |
8 |
3.907137696 |
1.51299E+01 |
8 |
4.659780505 |
2.48960E+01 |
8 |
4.007233994 |
1.59704E+01 |
8 |
4.710078203 |
2.62970E+01 |
8 |
4.107360133 |
1.69311E+01 |
8 |
4.760314859 |
2.81780E+01 |
8 |
4.207682570 |
1.79317E+01 |
8 |
4.810536961 |
3.01400E+01 |
8 |
4.307978467 |
1.91320E+01 |
>
8 |
4.860791389 |
3.29010E+01 |
8 |
4.408382309 |
2.04530E+01 |
8 |
4.911025444 |
3.61430E+01 |
8 |
4.508963741 |
2.20140E+01 |
8 |
4.961186960 |
4.04260E+01 |
8 |
4.559218620 |
2.28950E+01 |
8 |
5.011324184 |
4.60300E+01 |
8 |
4.609475809 |
2.37750E+01 |
8 |
5.061435817 |
5.40350E+01 |
8 |
Table
7.2. Knots and coefficients for the spline fit of log10 Cs
for T < T
Knots |
Coefficients |
K(1)
= 1.00000000000E-2 |
C(1)
= -7.080029E+0 |
K(2)
= 1.00000000000E-2 |
C(2)
= -6.461204E+0 |
K(3)
= 1.00000000000E-2 |
C(3)
= -5.407887E+0 |
K(4)
= 1.00000000000E-2 |
C(4)
= -4.971098E+0 |
K(5)
= 2.49738990740E-2 |
C(5)
= -4.092648E+0 |
K(6)
= 6.07641105990E-2 |
C(6)
= -3.430290E+0 |
K(7)
= 6.36528653770E-2 |
C(7)
= -2.300493E+0 |
K(8)
= 1.54157179076E-1 |
C(8)
= -1.865551E+0 |
K(9)
= 2.49299135447E-1 |
C(9)
= -6.120157E-1 |
K(10)
= 6.34497077644E-1 |
C(10)
= 1.800753E-1 |
K(11)
= 9.04465380669E-1 |
C(11)
= 8.200057E-1 |
K(12)
= 1.17474564385E+0 |
C(12)
= 1.231093E+0 |
K(13)
= 1.54255910867E+0 |
C(13)
= 1.494099E+0 |
K(14)
= 2.06499088720E+0 |
C(14)
= 1.633977E+0 |
K(15)
= 2.16070930746E+0 |
C(15)
= 1.694854E+0 |
K(16)
= 2.17157525125E+0 |
C(16)
= 1.760367E+0 |
K(17)
= 2.17590629200E+0 |
C(17)
= 1.813528E+0 |
K(18)
= 2.17655315900E+0 |
C(18)
= 1.849639E+0 |
K(19)
= 2.17672849900E+0 |
C(19)
= 1.900049E+0 |
K(20)
= 2.17678788100E+0 |
C(20)
= 1.935770E+0 |
K(21)
= 2.17679663200E+0 |
C(21)
= 1.974983E+0 |
K(22)
= 2.17679958200E+0 |
C(22)
= 2.017442E+0 |
K(23)
= 2.17679996468E+0 |
|
K(24)
= 2.17679996468E+0 |
|
K(25)
= 2.17679996468E+0 |
|
K(26)
= 2.17679996468E+0 |
|
.Table
7.3. Knots and coefficients for the spline fit of log10 Cs
for T > T.
Knots |
Coefficients |
K(1)
= 2.17680013200E+0 |
C(1)
= 1.900539E+0 |
K(2)
= 2.17680013200E+0 |
C(2)
= 1.862865E+0 |
K(3)
= 2.17680013200E+0 |
C(3)
= 1.822431E+0 |
K(4)
= 2.17680013200E+0 |
C(4)
= 1.759056E+0 |
K(5)
= 2.17680101200E+0 |
C(5)
= 1.679157E+0 |
K(6)
= 2.17680349500E+0 |
C(6)
= 1.584631E+0 |
K(7)
= 2.17681801800E+0 |
C(7) = 1.464344E+0 |
K(8)
= 2.17692420600E+0 |
C(8)
= 1.274043E+0 |
K(9)
= 2.17750755600E+0 |
C(9) = 1.095050E+0 |
K(10)
= 2.18086397100E+0 |
C(10)
= 9.546039E-1 |
K(11)
= 2.20374020794E+0 |
C(11)
= 9.503531E-1 |
K(12)
= 2.30368058865E+0 |
C(12)
= 1.100724E+0 |
K(13)
= 2.60849038128E+0 |
C(13)
= 1.260996E+0 |
K(14)
= 3.60335763894E+0 |
C(14)
= 1.421360E+0 |
K(15)
= 4.41358469422E+0 |
C(15)
= 1.609738E+0 |
K(16)
= 4.81404577042E+0 |
C(16) = 1.732672E+0 |
K(17)
= 5.06143581698E+0 |
|
K(18)
= 5.06143581698E+0 |
|
K(19)
= 5.06143581698E+0 |
|
K(20)
= 5.06143581698E+0 |
|
Table 7.4. Recommended values
of the heat capacity of liquid 4He
T90 (K) |
Cs (J/mol·K) |
T90 (K) |
Cs (J/mol·K) |
0.0000
|
0
|
2.2000
|
1.673E+1 |
0.0500
|
1.023E-05 |
2.2500
|
1.228E+1 |
0.1000
|
8.250E-05
|
2.3000
|
1.078E+1 |
0.1500
|
2.824E-4
|
2.3500
|
1.001E+1 |
0.2000
|
6.597E-4
|
2.4000
|
9.515E+0 |
0.2500
|
1.267E-3
|
2.4500
|
9.225E+0 |
0.3000
|
2.172E-3 |
2.5000
|
9.083E+0 |
0.3500
|
3.431E-3 |
2.5500
|
9.043E+0 |
0.4000
|
5.086E-3
|
2.6000
|
9.066E+0 |
0.4500
|
7.206E-3
|
2.6500
|
9.117E+0 |
0.5000
|
9.939E-3
|
2.7000 |
9.186E+0 |
0.5500
|
1.359E-2
|
2.7500
|
9.271E+0 |
0.6000
|
1.877E-2
|
2.8000
|
9.374E+0 |
0.6500
|
2.665E-2
|
2.8500 |
9.493E+0 |
0.7000
|
3.919E-2
|
2.9000 |
9.628E+0 |
0.7500
|
5.901E-2 |
2.9500
|
9.778E+0 |
0.8000
|
8.976E-2
|
3.0000
|
9.944E+0 |
0.8500
|
1.361E-1
|
3.0500
|
1.012E+1 |
0.9000
|
2.030E-1 |
3.1000
|
1.032E+1 |
0.9500
|
2.946E-1
|
3.1500 |
1.053E+1 |
1.0000
|
4.154E-1
|
3.2000
|
1.075E+1 |
1.0500
|
5.707E-1
|
3.2500
|
1.099E+1 |
1.1000
|
7.658E-1
|
3.3000
|
1.124E+1 |
1.1500
|
1.006E+0
|
3.3500 |
1.151E+1 |
1.2000
|
1.297E+0
|
3.4000
|
1.178E+1 |
1.2500
|
1.646E+0
|
3.4500 |
1.207E+1 |
1.3000
|
2.057E+0
|
3.5000
|
1.237E+1 |
1.3500 |
2.537E+0 |
3.5500
|
1.268E+1 |
1.4000 |
3.092E+0 |
3.6000
|
1.300E+1 |
1.4500
|
3.732E+0 |
3.6500
|
1.333E+1 |
1.5000
|
4.468E+0
|
3.7000
|
1.366E+1 |
1.5500
|
5.313E+0
|
3.7500 |
1.401E+1 |
1.6000
|
6.285E+0
|
3.8000
|
1.437E+1 |
1.6500
|
7.401E+0
|
3.8500 |
1.475E+1 |
1.7000
|
8.678E+0
|
3.9000
|
1.513E+1 |
1.7500 |
1.014E+1 |
3.9500 |
1.554E+1 |
1.8000
|
1.181E+1
|
4.0000
|
1.596E+1 |
1.8500
|
1.372E+1
|
4.0500
|
1.640E+1 |
1.9000
|
1.590E+1 |
4.1000
|
1.687E+1 |
1.9500
|
1.841E+1 |
4.1500 |
1.736E+1 |
2.0000
|
2.128E+1
|
4.2000
|
1.788E+1 |
2.0500
|
2.459E+1
|
4.2500 |
1.84E+01 |
2.1000
|
2.864E+1
|
4.3000 |
1.90E+01 |
2.1500 |
3.689E+1 |
4.3500 |
1.96E+01 |
2.1760
|
5.569E+1 |
4.4000
|
2.03E+01 |
2.1761
|
5.623E+1
|
4.4500
|
2.10E+01 |
2.1762
|
5.692E+1 |
4.5000
|
2.18E+01 |
2.1763
|
5.784E+1
|
4.5500
|
2.26E+01 |
2.1764
|
5.906E+1
|
4.6000 |
2.36E+01 |
2.1765
|
6.068E+1 |
4.6500 |
2.48E+01 |
2.1766
|
6.283E+1 |
4.7000
|
2.61E+01 |
2.1767
|
6.640E+1
|
4.7500 |
2.78E+01 |
2.1768
|
-
|
4.8000
|
2.98E+01 |
2.1769
|
4.569E+1
|
4.8500
|
3.22E+01 |
2.1770
|
4.227E+1
|
4.9000
|
3.53E+01 |
2.1775
|
3.543E+1 |
4.9500
|
3.93E+01 |
2.1780
|
3.264E+1
|
5.0000
|
4.47E+01 |
Table
7.5. Knots and coefficients for the spline fit to the enthalpy of liquid
4He.
Knots |
Coefficients |
K(1)=0.000000 |
C(1)=0.000000E+00 |
K(2)=0.000000 |
C(2)=0.000000E+00 |
K(3)=0.000000
|
C(3)=-1.650000E-06 |
K(4)=0.000000
|
C(4)=1.801000E-05 |
K(5)=0.100000 |
C(5)=1.185000E-04 |
K(6)=0.200000
|
C(6)=4.108550E-04 |
K(7)=0.300000
|
C(7)=1.033200E-03 |
K(8)=0.370000
|
C(8)=2.710000E-03 |
K(9)=0.500000
|
C(9)=6.090000E-03 |
K(10)=0.610000
|
C(10)=1.784000E-02 |
K(11)=0.743950
|
C(11)=6.032740E-02 |
K(12)=0.870000
|
C(12)=2.400500E-01 |
K(13)=1.027550
|
C(13)=8.643720E-01 |
K(14)=1.250000
|
C(14)=2.445400E+00 |
K(15)=1.500000
|
C(15)=5.554360E+00 |
K(16)=1.750000
|
C(16)=8.800000E+00 |
K(17)=2.000000
|
C(17)=1.220130E+01 |
K(18)=2.130000
|
C(18)=1.558100E+01 |
K(19)=2.190120
|
C(19)=2.004000E+01 |
K(20)=2.232940
|
C(20)=3.223100E+01 |
K(21)=2.854200
|
C(21)=4.704640E+01 |
K(22)=4.000000
|
C(22)=5.848930E+01 |
K(23)=4.900000 |
|
K(24)=4.900000 |
|
K(25)=4.900000 |
|
K(26)=4.900000 |
|
Table
7.6. Recommended values of the enthalpy of liquid 4He.
T90 (K) |
H (J mol-1) |
T90 (K) |
H (J mol-1) |
0.10
|
2.039E-06
|
2.60
|
16.876 |
0.15
|
1.056E-05
|
2.65 |
17.332 |
0.20
|
3.334E-05
|
2.70 |
17.784 |
0.25
|
8.018E-05
|
2.75 |
18.237 |
0.30
|
1.651E-04
|
2.80 |
18.696 |
0.35
|
3.035E-04
|
2.85
|
19.168 |
0.40
|
5.130E-04
|
2.90 |
19.656 |
0.45
|
8.178E-04
|
2.95
|
20.162 |
0.50
|
1.250E-03
|
3.00
|
20.686 |
0.55
|
1.840E-03
|
3.05 |
21.228 |
0.60
|
2.640E-03
|
3.10
|
21.789 |
0.65
|
3.740E-03
|
3.15
|
22.367 |
0.70
|
5.370E-03
|
3.20 |
22.964 |
0.75
|
7.830E-03
|
3.25 |
23.580 |
0.80
|
1.152E-02
|
3.30
|
24.213 |
0.85
|
1.713E-02
|
3.35
|
24.866 |
0.90 |
2.543E-02 |
3.40
|
25.537 |
0.95
|
3.765E-02
|
3.45 |
26.227 |
1.00 |
5.535E-02 |
3.50
|
26.935 |
1.05
|
8.014E-02
|
3.55 |
27.662 |
1.10
|
1.140E-01
|
3.60 |
28.409 |
1.15
|
1.591E-01
|
3.65
|
29.174 |
1.20 |
2.180E-01 |
3.70 |
29.958 |
1.25
|
2.928E-01
|
3.75
|
30.762 |
1.30
|
3.863E-01
|
3.80 |
31.584 |
1.35
|
5.020E-01
|
3.85 |
32.426 |
1.40
|
6.436E-01
|
3.90 |
33.288 |
1.45
|
8.150E-01
|
3.95 |
34.168 |
1.50
|
1.020 |
4.00 |
35.069 |
1.55 |
1.263 |
4.05
|
35.989 |
1.60
|
1.553
|
4.10
|
36.933 |
1.65
|
1.899 |
4.15 |
37.905 |
1.70
|
2.311
|
4.20
|
38.908 |
1.75
|
2.799
|
4.25 |
39.946 |
1.80
|
3.370 |
4.30
|
41.024 |
1.85 |
4.028 |
4.35
|
42.146 |
1.90 |
4.775 |
4.40
|
43.315 |
1.95 |
5.615 |
4.45
|
44.535 |
2.00
|
6.548
|
4.50
|
45.811 |
2.05
|
7.607
|
4.55
|
47.146 |
2.10
|
8.945
|
4.60 |
48.545 |
2.15
|
10.724
|
4.65 |
50.011 |
2.20
|
12.340
|
4.70
|
51.548 |
2.25 |
13.104 |
4.75 |
53.160 |
2.30
|
13.743 |
4.80 |
54.852 |
2.35 |
14.340 |
4.85 |
56.627 |
2.40
|
14.899
|
4.90
|
58.489 |
2.45
|
15.427
|
4.95
|
60.443 |
2.50 |
15.929 |
5.00 |
62.491 |
2.55
|
16.410 |
|
|
Chronological
Bibliography for Heat Capacity and Enthalpy
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 |
R.
W. Hill and O. V. Lounasmaa, “The Specific Heat of Liquid Helium,”
Philos. Mag. 2, 143-148 (1957). |
4 |
W.
M. Fairbank, M. J. Buckingham, and C. F. Keller, “Specific Heat
of Liquid 4He Near the Lambda Point,” in 5th International Conference
on Low Temperature Physics and Chemistry, edited by J. R. Dillinger
(1958), pp. 50-52. |
5 |
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). |
6 |
M.
J. Buckingham and W. M. Fairbank, “The Nature of the Lambda
Transition in Liquid Helium,” in Progress in Low Temperature
Physics, edited by C. G. Gorter (North Holland Publishing, 1961),
Vol. 3, pp. 80-112. |
7 |
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). |
8 |
W.
M. Fairbank, “The Nature of the Lambda Transition in Liquid
Helium,” in International School of Physics, Course XXI, edited
by G. Careri (New York: Academic Press, 1963). |
9 |
J.
Wiebes, “Caloric Measurements on Liquid and Melting Helium Below
1.5 Kelvin,” Ph.D. Thesis, Kammerlingh Onnes Laboratory, 1969
(unpublished). |
10 |
N.
E. Phillips, C. G. Waterfield, and J. K. Hoffer, “Calorimetric
Evidence for Positive Phonon Dispersion in Liquid 4He,” Phys.
Rev. Lett. 25, 1260 (1970). |
11 |
G.
Ahlers, “Heat Capacity Near the Superfluid Transition in 4He
at the Saturated Vapor Pressure,” Phys. Rev. A 3, 696-716 (1971). |
12 |
S.
A. Scott, E. Guyon, and I. Rudnick, “Specific Heat and Superfluid
Density of Liquid Helium in Porous Media,” J. Low. Temp. Phys.
9, 389-407 (1972). |
13 |
G.
Ahlers, “Thermodynamics and Experimental Tests of Static Scaling
and Universality Near the Superfluid Transition in 4He Under Pressure,”
Phys. Rev. A 8, 530-568 (1973). |
14 |
R.
J. Donnelly and P. H. Roberts, “A Theory of Temperature-Dependent
Energy Levels: Thermodynamic Properties of Helium II,” J. Low
Temp. Phys. 27, 687-736 (1977). |
15 |
D.
S. Greywall, “Specific Heat and Phonon Dispersion Curve of Liquid
4He,” Phys. Rev. B 18, 2127-214 (1978). |
16 |
D.
S. Greywall, “Erratum: Specific Heat and Phonon Dispersion Curve
of Liquid 4He,” Phys. Rev. B 21, 1329-1331 (1979). |
17 |
J.
A. Lipa and T. C. P. Chui, “Very High Resolution Heat-Capacity
Measurements Near the Lambda Point of Helium,” Phys. Rev. Lett.
51, 2291-2294 (1983). |
18 |
J.
A. Lipa, D. R. Swanson, J. A. Nissen, T. C. P. Chui, and U. E. Israelsson,
“Heat Capacity and Thermal Relaxation of Bulk Helium Very Near
the Lambda Point,” Phys. Rev. Letters 76, 944 (1996). |
|
|