Two balls of mass m1=m2=2kg have velocities v1=(3,0) and v2=(−5,4). Assuming (fancifully) that they form a monatomic ideal gas, calculate the associated “temperature”.
Solution
CM velocity:vCM=(23−5,20+4)=(−1,2)m/s
Velocities relative to the CM (vi′=vi−vCM):
v1′=(3,0)−(−1,2)=(4,−2),v2′=(−5,4)−(−1,2)=(−4,2)
As expected, m1v1′+m2v2′=0: the momentum in the CM frame is zero.
Internal kinetic energy (with ∣vi′∣2=42+22=20 for both):
Ecin,int=21⋅2⋅(16+4)+21⋅2⋅(16+4)=20+20=40J
Equivalent temperature (monatomic gas, Ecin,int=23NkBT, with N=2):
T=3NkB2Ecin,int=3⋅2⋅1,38⋅10−232⋅40=8,28⋅10−2380
T≈9,7⋅1023K
Astronomical! But this is an artefact of the toy model: with only N=2 particles, sharing out 40J means an enormous energy per particle. With a real gas of ∼1023 particles at speeds of a few m/s, the same formula would give a reasonable temperature.