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Question: Find the position of centre of mass from the base of a solid hemisphere of radius (A) \[16cm\] (B)...

Find the position of centre of mass from the base of a solid hemisphere of radius (A) 16cm16cm
(B) 4cm4cm
(C) 6cm6cm
(D) 8cm8cm
(E) 12cm12cm

Explanation

Solution

To solve this question, we need to find out the coordinates of the centre of mass with respect to the base. For this, divide the hemisphere into circular discs and find the centre of mass using integration, taking the origin at the base.
Formula Used: The formula used in this solution is
rcom=rdmdm{r_{com}} = \dfrac{{\int {rdm} }}{{\int {dm} }}, where dmdmis the mass of the elementary element,rris the position of the elementary element, and rcom{r_{com}}is the position of the centre of mass.

Complete step-by-step solution
Consider a solid hemisphere of radiusRR, massMM, and density ρ\rho as shown in the figure below.

As the hemisphere is symmetrical about the yyaxis, the xx coordinate of the centre of mass is00, i.e.
xcom=0{x_{com}} = 0
As the hemisphere is solid, we divide it into circular discs. Consider an elementary disc of xxradius at a height yy having thickness dydy as shown in the figure above.
The mass of the disc ==Volume of the disc ×\timesDensity
dm=ρdvdm = \rho dv (i)
whereρ\rho is the density of the hemisphere and dvdvis the elementary volume of the disc
Now, ρ=Mass of hemisphereVolume\rho = \dfrac{{Mass{\text{ }}of{\text{ }}hemisphere}}{{Volume}}
We know that Volume of hemisphere, V=23πR3V = \dfrac{2}{3}\pi {R^3}
ρ=M23πR3\therefore \rho = \dfrac{M}{{\dfrac{2}{3}\pi {R^3}}}
Which gives
ρ=3M2πR3\rho = \dfrac{{3M}}{{2\pi {R^3}}} (ii)
Now, Volume of the disc = Area of the disc ×\times Thickness
dv=πx2dy\therefore dv = \pi {x^2}dy (iii)
In the triangle AOBAOB, by Pythagoras theorem
OB2=OA2+AB2O{B^2} = O{A^2} + A{B^2}
From the figure we have
OB=ROB = R, OA=yOA = y and AB=xAB = x
R2=y2+x2\therefore {R^2} = {y^2} + {x^2}
Subtracting y2{y^2}from both the sides
x2=R2y2{x^2} = {R^2} - {y^2}
x=R2y2x = \sqrt {{R^2} - {y^2}} (iv)
\therefore from (i) we have
dm=ρdvdm = \rho dv
Substituting dvdv from (iii)
dm=ρ(πx2dy)dm = \rho (\pi {x^2}dy)
Substituting xx from (iv)
dm=ρ(π(R2y2)dy)dm = \rho (\pi ({R^2} - {y^2})dy)
Now, as we know the yy -coordinate of the centre of mass is given by
rcom=rdmdm{r_{com}} = \dfrac{{\int {rdm} }}{{\int {dm} }}
Substituting dm=ρ(π(R2y2)dy)dm = \rho (\pi ({R^2} - {y^2})dy)
ycom=yρπ(R2y2)dyM{y_{com}} = \dfrac{{\int {y\rho \pi ({R^2} - {y^2})dy} }}{M} (We know that dm=M\int {dm} = M)
As yy varies from 00 to RR in the figure above, we have
ycom=1M0Ryρπ(R2y2)dy{y_{com}} = \dfrac{1}{M}\int\limits_0^R {y\rho \pi ({R^2} - {y^2})dy}
As ρ\rho and π\pi are constants, we can take them out
ycom=ρπM0Ry(R2y2)dy{y_{com}} = \dfrac{{\rho \pi }}{M}\int\limits_0^R {y({R^2} - {y^2})dy}
ycom=ρπM0R(R2yy3)dy{y_{com}} = \dfrac{{\rho \pi }}{M}\int\limits_0^R {({R^2}y - {y^3})dy}
Separating into two integrals
ycom=ρπM(0RR2ydy0Ry3dy){y_{com}} = \dfrac{{\rho \pi }}{M}\left( {\int\limits_0^R {{R^2}ydy - \int\limits_0^R {{y^3}dy} } } \right)
Taking R2{R^2} outside as constant
ycom=ρπM(R20Rydy0Ry3dy){y_{com}} = \dfrac{{\rho \pi }}{M}\left( {{R^2}\int\limits_0^R {ydy - \int\limits_0^R {{y^3}dy} } } \right)
Performing integration, we get
ycom=ρπM(R2[y22]0R[y44]0R){y_{com}} = \dfrac{{\rho \pi }}{M}\left( {{R^2}\left[ {\dfrac{{{y^2}}}{2}} \right]_0^R - \left[ {\dfrac{{{y^4}}}{4}} \right]_0^R} \right)
Substituting the limits, we have
ycom=ρπM(R2[R22022][R44044]){y_{com}} = \dfrac{{\rho \pi }}{M}\left( {{R^2}\left[ {\dfrac{{{R^2}}}{2} - \dfrac{{{0^2}}}{2}} \right] - \left[ {\dfrac{{{R^4}}}{4} - \dfrac{{{0^4}}}{4}} \right]} \right)
ycom=ρπM(R42R44){y_{com}} = \dfrac{{\rho \pi }}{M}\left( {\dfrac{{{R^4}}}{2} - \dfrac{{{R^4}}}{4}} \right)
On simplifying
ycom=ρπM(R44){y_{com}} = \dfrac{{\rho \pi }}{M}\left( {\dfrac{{{R^4}}}{4}} \right)
Substituting ρ\rho from (ii), we get
ycom=3M2πR3πM(R44){y_{com}} = \dfrac{{3M}}{{2\pi {R^3}}}\dfrac{\pi }{M}\left( {\dfrac{{{R^4}}}{4}} \right)
Finally on simplifying, we get
ycom=3R8{y_{com}} = \dfrac{{3R}}{8}
Hence, the yy -coordinate of the centre of mass of the hemisphere is 3R8\dfrac{{3R}}{8}
This yy -coordinate is equal to the position of the COM from the base of the hemisphere, as the origin OO is taken on the base.
Thus, the position of the centre of mass from the base is given by
y=3R8y = \dfrac{{3R}}{8}
According to the question, R=16cmR = 16cm
Substituting this, we get
y=3(16)8y = \dfrac{{3(16)}}{8}
y=3(2)y = 3(2)
Finally,
y=6cmy = 6cm
So, the position of the centre of mass from the base of the hemisphere is 6cm6cm

Hence, the correct answer is option B, 6cm6cm

Note: Always prefer to use as small a number of variables as possible for performing integration. If the number of the variables is more, you may perform the integration incorrectly. To avoid this, convert all the variables in terms of one variable before putting them into the integral.