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Question: A solid hemisphere of radius R is mounted on a solid cylinder of the same radius and density as show...

A solid hemisphere of radius R is mounted on a solid cylinder of the same radius and density as shown. The height of the cylinder is such that the resulting centre of the mass is O. If the radius of the sphere is 22m2\sqrt{2}m and the height of the cylinder is n metre. Find n.

Explanation

Solution

Hint: Make the point O, which is the centre of mass of the system, as the origin (0,0). Then use the formula for centre of mass of a system of two bodies i.e Mxcom=M1x1+M2x2M{{x}_{com}}={{M}_{1}}{{x}_{1}}+{{M}_{2}}{{x}_{2}}, where M is total mass of the system, xcom is the position of centre of mass of the system, x1x_1 and x2x_2 are the positions of the centre of masses of M1M_1 and M2M_2.

Complete step by step answer:
The centre of mass for a solid hemisphere is at a distance of 3R8\dfrac{3R}{8} units from the centre of the circular base along the axis passing through this centre and perpendicular to the circular base. The centre of mass of a cylinder is at its centre i.e. at a distance of half of the height from the centre of the circular and perpendicular to the surface of the top.
We know the centre of mass of the hemisphere and the cylinder. Let the mass of the hemisphere be M1 and the mass of the cylinder be M2. Then by using the centre of mass formula Mxcom=M1x1+M2x2M{{x}_{com}}={{M}_{1}}{{x}_{1}}+{{M}_{2}}{{x}_{2}} ……(1) , where M is total mass of the system, xcom is the position of centre of mass of the system, x1x_1 and x2x_2 are the positions of the centre of masses of M1M_1 and M2M_2. In this case, M=M1+M2M={{M}_{1}}+{{M}_{2}}…….(2). Let the origin (0,0) be point O and also it is given to the centre of mass of the system. xcom=0\Rightarrow {{x}_{com}}=0.
x1=3R8{{x}_{1}}=\dfrac{3R}{8} and we have to find x2x_2. Before that let us find M1M_1 and M2M_2.
The hemisphere and the cylinder have the same radius (R) and same density (ρ\rho ). The formula for density is  !!ρ!! =massvolume\text{ }\\!\\!\rho\\!\\!\text{ =}\dfrac{\text{mass}}{\text{volume}} . Therefore,  !!ρ!! =massvolume=M1V1=M2V2\text{ }\\!\\!\rho\\!\\!\text{ =}\dfrac{\text{mass}}{\text{volume}}=\dfrac{{{M}_{1}}}{{{V}_{1}}}=\dfrac{{{M}_{2}}}{{{V}_{2}}}, where V1V_1 and V2V_2 are the volumes of the hemisphere and the cylinder respectively.
V2=23πR3\Rightarrow {{V}_{2}}=\dfrac{2}{3}\pi {{R}^{3}} and V2=πR2h\Rightarrow {{V}_{2}}=\pi {{R}^{2}}h (h is the height of the cylinder)
M1=ρV1=23ρπR3\Rightarrow {{M}_{1}}=\rho {{V}_{1}}=\dfrac{2}{3}\rho \pi {{R}^{3}} and M2=ρV2=ρπR2h{{M}_{2}}=\rho {{V}_{2}}=\rho \pi {{R}^{2}}h
Substitute the values of M1 and M2 in equation (2).
M=23ρπR3+ρπR2h\Rightarrow M=\dfrac{2}{3}\rho \pi {{R}^{3}}+\rho \pi {{R}^{2}}h
Substitute the values of M, M1 and M2 in equation (1).
Therefore, (23ρπR3+ρπR2h)xcom=23ρπR3x1+ρπR2hx2\left( \dfrac{2}{3}\rho \pi {{R}^{3}}+\rho \pi {{R}^{2}}h \right){{x}_{com}}=\dfrac{2}{3}\rho \pi {{R}^{3}}{{x}_{1}}+\rho \pi {{R}^{2}}h{{x}_{2}}
We had assumed xcom to be 0. x1=3R8{{x}_{1}}=\dfrac{3R}{8}. Substitute these values in the above equation.
(23ρπR3+ρπR2h).(0)=23ρπR3.(3R8)+ρπR2hx2\Rightarrow \left( \dfrac{2}{3}\rho \pi {{R}^{3}}+\rho \pi {{R}^{2}}h \right).(0)=\dfrac{2}{3}\rho \pi {{R}^{3}}.\left( \dfrac{3R}{8} \right)+\rho \pi {{R}^{2}}h{{x}_{2}}
(0)=R24+hx2\Rightarrow (0)=\dfrac{{{R}^{2}}}{4}+h{{x}_{2}}
Therefore, x2=R24h{{x}_{2}}=-\dfrac{{{R}^{2}}}{4h}. But we know that x2 will be half of the height of the cylinder. But since it is down the origin, the value of x2 will be negative. This implies, x2=h2{{x}_{2}}=-\dfrac{h}{2}
h2=R24hh2=R22\Rightarrow -\dfrac{h}{2}=-\dfrac{{{R}^{2}}}{4h}\Rightarrow {{h}^{2}}=\dfrac{{{R}^{2}}}{2}
Therefore, h=R2=222=2mh=\dfrac{R}{\sqrt{2}}=\dfrac{2\sqrt{2}}{\sqrt{2}}=2m. Hence, the height of the cylinder i.e. n is 2m.

Note: Here, there were only two bodies so the centre of mass of the system will be on the joining the centre of masses of both the bodies. If there are more bodies then we have to solve the question using vectors i.e. Mrcom=M1r1+M2r2+M3r3+.......M{{\overrightarrow{r}}_{com}}={{M}_{1}}{{\overrightarrow{r}}_{1}}+{{M}_{2}}{{\overrightarrow{r}}_{2}}+{{M}_{3}}{{\overrightarrow{r}}_{3}}+........