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Question: What is the radius of a steel sphere that will float on water with exactly half the sphere submerged...

What is the radius of a steel sphere that will float on water with exactly half the sphere submerged? Density of steel is 7.9×103kgm37.9 \times {10^3}\dfrac{{kg}}{{{m^3}}} and surface tension of water is 7×102N7 \times {10^{ - 2}}N.

Explanation

Solution

Forces on the sphere will be FT+FU=W{F_T} + {F_U} = W
FT{F_T} is the surface tension, FU{F_U} is the upthrust, WW is the weight of the sphere.
putting their respective values in the above equation we will find the radius of the steel sphere.

Formula used:
FT=2πr×T{F_T} = 2\pi r \times T where TT is the surface tension multiplied by the total length of the sphere in contact with water i.e. circumference of the circle.
FU=ρwgV{F_U} = {\rho _w}gV where ρw{\rho _w} is fluid density gg is the acceleration due to gravity VV is the volume of the object immersed.
W=VSρSgW = {V_S}{\rho _S}g where VS{V_S} is the volume of the sphere ρS{\rho _S} is the density of the sphere.

Complete step by step answer:

Here a steel sphere is half-submerged in water. FT{F_T} is the surface tension caused by water on the sphere. FU{F_U} is the up thrust experienced by the sphere. WW is the weight of the steel sphere.
Because it is half-submerged the forces will be balanced
Therefore, FT+FU=W{F_T} + {F_U} = W
FT=2πr×T{F_T} = 2\pi r \times T where TT is the surface tension multiplied by the total length of the sphere in contact with water i.e. circumference of the circle.
FU=ρwgV{F_U} = {\rho _w}gV where ρw{\rho _w} is fluid density gg is the acceleration due to gravity VV is the volume of the object immersed i.e. of hemisphere 23πr3\dfrac{2}{3}\pi {r^3}.
W=VSρSgW = {V_S}{\rho _S}g where VS{V_S} is the volume of the sphere 43πr3\dfrac{4}{3}\pi {r^3}, ρS{\rho _S} is the density of the sphere
2πr×T+23πr3×ρw×g=43πr3×ρs×g\Rightarrow 2\pi r \times T + \dfrac{2}{3}\pi {r^3} \times {\rho _w} \times g = \dfrac{4}{3}\pi {r^3} \times {\rho _s} \times g
T=r23×g(2ρsρw)\Rightarrow T = \dfrac{{{r^2}}}{3} \times g\left( {2{\rho _s} - {\rho _w}} \right)
ρS{\rho _S} is given in the question and the density of water is 11
r2=3Tg(2ρsρw)\Rightarrow {r^2} = \dfrac{{3T}}{{g(2{\rho _s} - {\rho _w})}}
7×102×310×(15.81)×103\Rightarrow \dfrac{{7 \times {{10}^{ - 2}} \times 3}}{{10 \times \left( {15.8 - 1} \right) \times {{10}^3}}}
r2=1.418×102\Rightarrow {r^2} = 1.418 \times {10^{ - 2}}
Hence the radius of the sphere is r=1.2×101cmr = 1.2 \times {10^{ - 1}}cm.

Note:
Any item submerged in a fluid or liquid, whether completely or partially, is buoyed up by a force equal to the weight of the fluid displaced by the object. When the surface of a sphere comes into contact with water, surface tension occurs. The upward force exerted by a fluid on an item is known as upthrust. That's why up-thrust works against an object's weight since it has displaced some water since it has half emerged; the sphere is experiencing up thrust.