In: Physics
A cylindrical glass beaker of height 1.272 m rests on a table. The bottom half of the beaker is filled with a gas, and the top half is filled with liquid mercury that is exposed to the atmosphere. The gas and mercury do not mix because they are separated by a frictionless, movable piston of negligible mass and thickness. The initial temperature is 276 K. The temperature is increased until a value is reached when one-half of the mercury has spilled out. Ignore the thermal expansion of the glass and mercury, and find this temperature in kelvins.
Given that :
initial temperature, T1 = 276 K
height of cylindrical beaker, h = 1.272 m
Ignore the thermal expansion of the glass and mercury.
using a combined gas laws,
P1 V1 / T1 = P2 V2 / T2 { eq.1 }
where, V = A d
then, P1 A d1 / T1 = P2 A d2 / T2
rearranging an above eq.
T2 = ( P2 / P1) (d2 / d1) T1 { eq.2 }
the initial pressure is given as :
P1 = P + gh1 { eq.3 }
where, P = constant pressure = 1.01 x 105 Pa
= density of mercury = 1.36 x 104 kg/m3
g = acceleration due to gravity = 9.8 m/s2
h1 = height of beaker = h / 2 = (1.272 m) / 2 = 0.636 m
inserting these values in eq.3,
P1 = (1.01 x 105 Pa) + (1.36 x 104 kg/m3) (9.8 m/s2) (0.636 m)
P1 = (1.01 x 105 Pa) + (8.47 x 104 Pa)
P1 = 185700 Pa
and final pressure is given as :
P2 = P + gh2 { eq.4 }
where, h2 = h1 / 2 = (0.636 m) / 2 = 0.318 m
P = constant pressure = 1.01 x 105 Pa
inserting the values in eq.4,
P2 = (1.01 x 105 Pa) + (1.36 x 104 kg/m3) (9.8 m/s2) (0.318 m)
P2 = (1.01 x 105 Pa) + (4.23 x 104 Pa)
P2 = 143300 Pa
Now, inserting all these values in eq.2,
T2 = ( P2 / P1) (d2 / d1) T1
T2 = [(143300 Pa) / (185700 Pa)] (d2 / d1) (276 K)
where, d1 = 0.636 m and d2 = (0.636 m) + (0.318 m) = 0.954 m
then, T2 = [(143300 Pa) / (185700 Pa)] [(0.954 m) / (0.636 m)] (276 K)
T2 = (0.7716) (1.5) (276 K)
T2 = 319.4 K