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Wineland image by James Burrus/NIST, courtesy of AIP Emilio Segrè
Visual Archives, W. F. Meggers Gallery of Nobel Laureates Collection
under the
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Commons CC0 1.0 Universal Public Domain Dedication License.
Schmidt image courtesy of Markus Pössel under the
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Commons Attribution-ShareAlike 3.0 Unported License.
Today is the birthday of
- David J. Wineland (1944-).
- Brian Schmidt (1967-).

Cormack image courtesy of
Landesarchiv
Baden-Württemberg, Fotograf: Willy Pragher under the
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Commons Attribution 3.0 Germany License.
Today is the birthday of
- Allan MacLeod Cormack (1924-1998).
- Johan Jakob Nervander (1805-1848).
Today’s Problem
Find the internal energy \(U\), enthalphy \(H\), entropy \(S\), Helmholtz free energy \(F\), and Gibbs free energy \(G\), for a mole of helium at atmospheric pressure \(P=1.013\times 10^5\,\text{N/m}^2\) and temperature \(T=298\)K.
Answer
We can assume helium is a monatomic ideal gas, so the internal energy is given by
\[U=\frac{3}{2}NkT = \frac{3}{2}(6.022\times 10^{23})(1.381\times 10^{-23}\,\text{J/K})(298\,\text{K})=3717.4\,\text{J}\]
Note that this is independent of the mass of the helium atom. It is the same for all monatomic ideal gases at \(T=298\) K.
The enthalpy is given by \(H=U+PV\). From the ideal gas law we have \(PV=NkT=\frac{2}{3}U\). So the enthalpy is simply proportional to the internal energy \(H=\frac{5}{3}U\).
To get the Helmholtz and Gibbs free energies we need to know the entropy. We can get that from the Sackur-Tetrode equation for the entropy of the monatomic ideal gas.
\[S=Nk\left[\ln\left(\frac{V}{N}\left(\frac{4\pi mU}{3Nh^2}\right)^{3/2}\right)+\frac{5}{2}\right]\]
Plugging in the numbers we get \(S=126\) J/K.
The Helmholtz free energy is given by \(F=U-TS\). Plugging in the numbers we get \(F=-33.8\) kJ.
The Gibbs free energy is given by \(G=H-TS\). Plugging in the numbers we get \(G=-31.4\) kJ.

Today is the birthday of
- Jean Charles Athanase Peltier (1785-1845).
- Heinrich
Hertz (1857-1894).
Get Heinrich Hertz merchandise.
Today is the birthday of
- Evgeny Lifshitz (1915-1985).
Today’s Problem
The enclosed volume of a Crookes radiometer is spherical with a diameter of 8 cm. At room temperature (20\(^{\circ}\)C), and a typical pressure of 13 Pa, estimate the number of air molecules in the radiometer.
Answer
Using the ideal gas law, \(PV=nRT\) where \(R=8.315\,\text{J}\cdot\text{mol}^{-1}\cdot\text{K}^{-1}\), we can get the number of moles, \(n=PV/(RT)\)
\[n = \frac{(13\,\text{J}\cdot\text{m}^{-3})(\frac{4}{3}\pi(0.08\,\text{m})^3)}{(8.315\,\text{J}\cdot\text{mol}^{-1}\cdot\text{K}^{-1})(273.15\,\text{K}+20\,\text{K})} = 1.14\times 10^{-5}\,\text{mol} = 11.4\,\mu\text{mol}\]
So the number of air molecules is
\[(1.14\times 10^{-5}\,\text{mol})(6.022\times 10^{23}\,\text{molecules/mole})=6.9\times 10^{18}\,\text{molecules}\]
© 2026 Stefan Hollos and Richard Hollos