1) Let us determine the density of the cylinder. The average density is
"\\rho = \\dfrac{m}{V}" , and in case of the cylinder the volume is
"V=\\pi \\dfrac{D^2}{4}h=\\pi\\cdot \\dfrac{(3.9\\,\\mathrm{cm})^2}{4}\\cdot3.9\\,\\text{cm} = 46.6\\,\\text{cm}^3."
Therefore, the density is
"\\rho =\\dfrac{1000\\,\\text{g}}{46.6\\,\\text{cm}^3} \\approx 21.5\\,\\text{g\/cm}^3."
2) First we determine the volume of the shell. It is equal to the difference between the volumes of bigger and smaller spheres:
"V = V_b-V_s = \\dfrac43\\pi (R_b^3-R_s^3) = \\dfrac43\\pi (5.75^3-5.70^3) = 20.59\\,\\text{cm}^3."
Therefore, the mass will be "m = \\rho V = 8.92\\,\\text{g\/cm}^3\\cdot20.59\\,\\text{cm}^3 = 183.66\\,\\text{g}."
3) "1\/32" inch = "1\/32\\cdot2.54\\,\\text{cm} = 7.9\\cdot10^{-2}\\,\\mathrm{cm} = 7.9\\cdot10^{-4}\\,\\mathrm{m} = 7.9\\cdot10^5\\,\\mathrm{nm}" per day.
There are "24\\cdot3600 = 86400" seconds in a day, so the rate is
"\\dfrac{7.9\\cdot10^5}{86400} = 9.2" nm/sec.
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