Explanations & Calculations
- The relationship between the height a particular liquid rises in a given capillary tube due to the surface tension is given by
"\\qquad\\qquad\n\\begin{aligned}\n\\small h &= \\small \\frac{2T\\cos\\theta }{r\\rho g}\\\\\n\n\\end{aligned}" : "\\small \\theta" is the contact angle between water & glass
- And for the given situation (10cm above the water level) the capillary rise is
"\\qquad\\qquad\n\\begin{aligned}\n\\small h_1 &= \\small \\frac{2\\times 0.072Nm^{-1}}{0.0002m \\times 10^3kgm^{-3}\\times 9.8ms^{-2}} \\cos\\theta\\\\\n\\small &= \\small 0.0735\\cos\\theta \\,\\,m \\\\\n\\small&=\\small 7.35\\cos \\theta \\,\\,cm\n\\end{aligned}"
- It's obvious that the capillary rise will not change as none of the components in the equation is changed even after the tube is depressed further.
- After it is depressed only 5 cm is above the water & if "\\small h_1<5cm" no water will spill & if "\\small h_1>>5cm" water will spill.
- If the capillary rise just a very little more that 5cm water will stay in the tube until the contact angle reaches 180 degrees without spill.
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