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Question: Consider the following statements Statement 1: CM of a uniform semicircular disc of radius \(R=\df...

Consider the following statements
Statement 1: CM of a uniform semicircular disc of radius R=2RπR=\dfrac{2R}{\pi } from the center.
Statement 2: CM of a uniform semicircular ring of radius R=4R3πR=\dfrac{4R}{3\pi } from the center.
Statement 3: CM of a solid hemisphere of radius R=4R3πR=\dfrac{4R}{3\pi } from the center.
Statement 4: CM of a hemisphere shell of radius R=R2R=\dfrac{R}{2} from the center.
Which statements are correct:
A) 1, 2, 4
B) 1, 3, 4
C) 4 only
D) 1, 2 only

Explanation

Solution

Calculate the CM for each of the mentioned masses from the method of integrating the mass and finding the center of mass. Take an infinitesimal element correspondingly and proceed accordingly.

Complete step by step solution:
For CM of a uniform semicircular ring, let us assume that the ring is kept in the y>0y>0 region. Let us consider dmdm at an angle θ\theta from the positive x-axis, which subtends an angle dθd\theta at the origin. The length of this dmdm is dl=Rdθdl=Rd\theta.
Length of a semicircular ring, l=πRl=\pi R
If mass for length l=Ml=M, then mass for length dl=Mldldl=\dfrac{M}{l}dl.
dm=MlRdθ\Rightarrow dm=\dfrac{M}{l}Rd\theta
Therefore, CMx=1M0πRcosθMπRRdθC{{M}_{x}}=\dfrac{1}{M}\int\limits_{0}^{\pi }{R\cos \theta \dfrac{M}{\pi R}}Rd\theta
CMx=0\Rightarrow C{{M}_{x}}=0
And, CMy=1M0πRsinθMπRRdθC{{M}_{y}}=\dfrac{1}{M}\int\limits_{0}^{\pi }{R\sin \theta \dfrac{M}{\pi R}}Rd\theta
CMy=2Rπ\Rightarrow C{{M}_{y}}=\dfrac{2R}{\pi }

For CM of a semicircular disc, let us assume that the disc is kept in the y>0y>0 region. Let us consider a ring on the disc of radius rr, of thickness drdr and mass dmdm.
Mass per unit area of the disc:
MA=M(πR22)=2MπR2\dfrac{M}{A}=\dfrac{M}{\left( \dfrac{\pi {{R}^{2}}}{2} \right)}=\dfrac{2M}{\pi {{R}^{2}}}
Area of the considered ring:
Ar=πrdr{{A}_{r}}=\pi rdr
Therefore, dm=MAAr=2MπR2πrdr=2MR2rdrdm=\dfrac{M}{A}{{A}_{r}}=\dfrac{2M}{\pi {{R}^{2}}}\pi rdr=\dfrac{2M}{{{R}^{2}}}rdr
Hence, CMy=1M0Mydm=1M0R2rπ2MR2rdrC{{M}_{y}}=\dfrac{1}{M}\int\limits_{0}^{M}{ydm=\dfrac{1}{M}\int\limits_{0}^{R}{\dfrac{2r}{\pi }}\dfrac{2M}{{{R}^{2}}}}rdr
CMy=4πR20Rr2dr=4R3πC{{M}_{y}}=\dfrac{4}{\pi {{R}^{2}}}\int\limits_{0}^{R}{{{r}^{2}}}dr=\dfrac{4R}{3\pi }

For CM of solid Hemisphere, let us assume that the hemisphere is kept in the y>0y>0 region. Let us assume a disc contained inside the hemisphere at a height yy, of thickness dydy and mass dmdm, with radius rr.
Mass per unit volume of the hemisphere:
MV=M(23πR3)=3M2πR3\dfrac{M}{V}=\dfrac{M}{\left( \dfrac{2}{3}\pi {{R}^{3}} \right)}=\dfrac{3M}{2\pi {{R}^{3}}}
Let the volume of the disc considered be dVdV.
dV=πr2dydV=\pi {{r}^{2}}dy
By applying Pythagoras theorem:
y2+r2=R2{{y}^{2}}+{{r}^{2}}={{R}^{2}} r2=R2y2\Rightarrow {{r}^{2}}={{R}^{2}}-{{y}^{2}}
Therefore, dV=π(R2y2)dydV=\pi \left( {{R}^{2}}-{{y}^{2}} \right)dy
dm=MVdV=3M2πR2π(R2y2)dydm=\dfrac{M}{V}dV=\dfrac{3M}{2\pi {{R}^{2}}}\pi ({{R}^{2}}-{{y}^{2}})dy
CMy=1M0Mydm=1M0Ry3M2R3(R2y2)dyC{{M}_{y}}=\dfrac{1}{M}\int\limits_{0}^{M}{ydm}=\dfrac{1}{M}\int\limits_{0}^{R}{y}\dfrac{3M}{2{{R}^{3}}}\left( {{R}^{2}}-{{y}^{2}} \right)dy
CMy=32R30R(yR2y3)dyC{{M}_{y}}=\dfrac{3}{2{{R}^{3}}}\int\limits_{0}^{R}{(y{{R}^{2}}-{{y}^{3}})}dy
CMy=3R8C{{M}_{y}}=\dfrac{3R}{8}

For the CM of a hemispherical shell, let us assume that the hemispherical shell is kept in the region y>0y>0. Let us consider a ring contained at the periphery of the shell at height yy, radius rr and subtends and dθd\theta at the origin, θ\theta is the angle at which the ring is considered from the x-axis. Therefore, the thickness of the ring is RdθRd\theta. Let the mass of this ring be dmdm .
Let dAdA be the surface area of the ring.
dA=2πrRdθdA=2\pi rRd\theta
From trigonometry, it can be easily proved that r=Rcosθr=R\cos \theta and y=Rsinθy=R\sin \theta .
dA=2πRcosθRdθ=2πR2cosθdθ\Rightarrow dA=2\pi R\cos \theta Rd\theta =2\pi {{R}^{2}}\cos \theta d\theta
Mass per unit area of the hemispherical shell:
MA=M2πR2\dfrac{M}{A}=\dfrac{M}{2\pi {{R}^{2}}}
dm=M2πR22πR2cosθdθ=Mcosθdθdm=\dfrac{M}{2\pi {{R}^{2}}}2\pi {{R}^{2}}\cos \theta d\theta =M\cos \theta d\theta
CMy=1M0Mydm=1M0π2RsinθMcosθdθC{{M}_{y}}=\dfrac{1}{M}\int\limits_{0}^{M}{ydm}=\dfrac{1}{M}\int\limits_{0}^{\dfrac{\pi }{2}}{R\sin \theta M\cos \theta d\theta }
CMy=R20π2sin(2θ)dθC{{M}_{y}}=\dfrac{R}{2}\int\limits_{0}^{\dfrac{\pi }{2}}{\sin (2\theta )d\theta }
CMy=R2C{{M}_{y}}=\dfrac{R}{2}
Therefore, only statement 4 is correct.

Hence, option (C) is correct.

Note: Do the integration very carefully as many errors can be done while doing integration. Don’t forget to write constants while doing integration. Take proper care of the limits of the integration. Do the manipulation(s) carefully, if required.