Consider the following statements
Statement 1: CM of a uniform semicircular disc of radius $R=\dfrac{2R}{\pi }$ from the center.
Statement 2: CM of a uniform semicircular ring of radius $R=\dfrac{4R}{3\pi }$ from the center.
Statement 3: CM of a solid hemisphere of radius $R=\dfrac{4R}{3\pi }$ from the center.
Statement 4: CM of a hemisphere shell of radius $R=\dfrac{R}{2}$ from the center.
Which statements are correct:
A) 1, 2, 4
B) 1, 3, 4
C) 4 only
D) 1, 2 only
Answer
298.5k+ views
Hint: 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 $y>0$ region. Let us consider $dm$ at an angle $\theta $ from the positive x-axis, which subtends an angle $d\theta $ at the origin. The length of this $dm$ is $dl=Rd\theta$.
Length of a semicircular ring, $l=\pi R$
If mass for length $l=M$, then mass for length $dl=\dfrac{M}{l}dl$.
$\Rightarrow dm=\dfrac{M}{l}Rd\theta $
Therefore, $C{{M}_{x}}=\dfrac{1}{M}\int\limits_{0}^{\pi }{R\cos \theta \dfrac{M}{\pi R}}Rd\theta $
$\Rightarrow C{{M}_{x}}=0$
And, $C{{M}_{y}}=\dfrac{1}{M}\int\limits_{0}^{\pi }{R\sin \theta \dfrac{M}{\pi R}}Rd\theta $
$\Rightarrow C{{M}_{y}}=\dfrac{2R}{\pi }$
For CM of a semicircular disc, let us assume that the disc is kept in the $y>0$ region. Let us consider a ring on the disc of radius $r$, of thickness $dr$ and mass $dm$.
Mass per unit area of the disc:
$\dfrac{M}{A}=\dfrac{M}{\left( \dfrac{\pi {{R}^{2}}}{2} \right)}=\dfrac{2M}{\pi {{R}^{2}}}$
Area of the considered ring:
${{A}_{r}}=\pi rdr$
Therefore, $dm=\dfrac{M}{A}{{A}_{r}}=\dfrac{2M}{\pi {{R}^{2}}}\pi rdr=\dfrac{2M}{{{R}^{2}}}rdr$
Hence, $C{{M}_{y}}=\dfrac{1}{M}\int\limits_{0}^{M}{ydm=\dfrac{1}{M}\int\limits_{0}^{R}{\dfrac{2r}{\pi }}\dfrac{2M}{{{R}^{2}}}}rdr$
$C{{M}_{y}}=\dfrac{4}{\pi {{R}^{2}}}\int\limits_{0}^{R}{{{r}^{2}}}dr=\dfrac{4R}{3\pi }$
For CM of solid Hemisphere, let us assume that the hemisphere is kept in the $y>0$ region. Let us assume a disc contained inside the hemisphere at a height $y$, of thickness $dy$ and mass $dm$, with radius $r$.
Mass per unit volume of the hemisphere:
$\dfrac{M}{V}=\dfrac{M}{\left( \dfrac{2}{3}\pi {{R}^{3}} \right)}=\dfrac{3M}{2\pi {{R}^{3}}}$
Let the volume of the disc considered be $dV$.
$dV=\pi {{r}^{2}}dy$
By applying Pythagoras theorem:
${{y}^{2}}+{{r}^{2}}={{R}^{2}}$ $\Rightarrow {{r}^{2}}={{R}^{2}}-{{y}^{2}}$
Therefore, $dV=\pi \left( {{R}^{2}}-{{y}^{2}} \right)dy$
$dm=\dfrac{M}{V}dV=\dfrac{3M}{2\pi {{R}^{2}}}\pi ({{R}^{2}}-{{y}^{2}})dy$
$C{{M}_{y}}=\dfrac{1}{M}\int\limits_{0}^{M}{ydm}=\dfrac{1}{M}\int\limits_{0}^{R}{y}\dfrac{3M}{2{{R}^{3}}}\left( {{R}^{2}}-{{y}^{2}} \right)dy$
$C{{M}_{y}}=\dfrac{3}{2{{R}^{3}}}\int\limits_{0}^{R}{(y{{R}^{2}}-{{y}^{3}})}dy$
$C{{M}_{y}}=\dfrac{3R}{8}$
For the CM of a hemispherical shell, let us assume that the hemispherical shell is kept in the region $y>0$. Let us consider a ring contained at the periphery of the shell at height $y$, radius $r$ and subtends and $d\theta$ at the origin, $\theta$ is the angle at which the ring is considered from the x-axis. Therefore, the thickness of the ring is $Rd\theta$. Let the mass of this ring be $dm$ .
Let $dA$ be the surface area of the ring.
$dA=2\pi rRd\theta $
From trigonometry, it can be easily proved that $r=R\cos \theta $ and $y=R\sin \theta $ .
$\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:
$\dfrac{M}{A}=\dfrac{M}{2\pi {{R}^{2}}}$
$dm=\dfrac{M}{2\pi {{R}^{2}}}2\pi {{R}^{2}}\cos \theta d\theta =M\cos \theta d\theta $
$C{{M}_{y}}=\dfrac{1}{M}\int\limits_{0}^{M}{ydm}=\dfrac{1}{M}\int\limits_{0}^{\dfrac{\pi }{2}}{R\sin \theta M\cos \theta d\theta }$
$C{{M}_{y}}=\dfrac{R}{2}\int\limits_{0}^{\dfrac{\pi }{2}}{\sin (2\theta )d\theta }$
$C{{M}_{y}}=\dfrac{R}{2}$
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.
Complete step by step solution:
For CM of a uniform semicircular ring, let us assume that the ring is kept in the $y>0$ region. Let us consider $dm$ at an angle $\theta $ from the positive x-axis, which subtends an angle $d\theta $ at the origin. The length of this $dm$ is $dl=Rd\theta$.
Length of a semicircular ring, $l=\pi R$
If mass for length $l=M$, then mass for length $dl=\dfrac{M}{l}dl$.
$\Rightarrow dm=\dfrac{M}{l}Rd\theta $
Therefore, $C{{M}_{x}}=\dfrac{1}{M}\int\limits_{0}^{\pi }{R\cos \theta \dfrac{M}{\pi R}}Rd\theta $
$\Rightarrow C{{M}_{x}}=0$
And, $C{{M}_{y}}=\dfrac{1}{M}\int\limits_{0}^{\pi }{R\sin \theta \dfrac{M}{\pi R}}Rd\theta $
$\Rightarrow C{{M}_{y}}=\dfrac{2R}{\pi }$
For CM of a semicircular disc, let us assume that the disc is kept in the $y>0$ region. Let us consider a ring on the disc of radius $r$, of thickness $dr$ and mass $dm$.
Mass per unit area of the disc:
$\dfrac{M}{A}=\dfrac{M}{\left( \dfrac{\pi {{R}^{2}}}{2} \right)}=\dfrac{2M}{\pi {{R}^{2}}}$
Area of the considered ring:
${{A}_{r}}=\pi rdr$
Therefore, $dm=\dfrac{M}{A}{{A}_{r}}=\dfrac{2M}{\pi {{R}^{2}}}\pi rdr=\dfrac{2M}{{{R}^{2}}}rdr$
Hence, $C{{M}_{y}}=\dfrac{1}{M}\int\limits_{0}^{M}{ydm=\dfrac{1}{M}\int\limits_{0}^{R}{\dfrac{2r}{\pi }}\dfrac{2M}{{{R}^{2}}}}rdr$
$C{{M}_{y}}=\dfrac{4}{\pi {{R}^{2}}}\int\limits_{0}^{R}{{{r}^{2}}}dr=\dfrac{4R}{3\pi }$
For CM of solid Hemisphere, let us assume that the hemisphere is kept in the $y>0$ region. Let us assume a disc contained inside the hemisphere at a height $y$, of thickness $dy$ and mass $dm$, with radius $r$.
Mass per unit volume of the hemisphere:
$\dfrac{M}{V}=\dfrac{M}{\left( \dfrac{2}{3}\pi {{R}^{3}} \right)}=\dfrac{3M}{2\pi {{R}^{3}}}$
Let the volume of the disc considered be $dV$.
$dV=\pi {{r}^{2}}dy$
By applying Pythagoras theorem:
${{y}^{2}}+{{r}^{2}}={{R}^{2}}$ $\Rightarrow {{r}^{2}}={{R}^{2}}-{{y}^{2}}$
Therefore, $dV=\pi \left( {{R}^{2}}-{{y}^{2}} \right)dy$
$dm=\dfrac{M}{V}dV=\dfrac{3M}{2\pi {{R}^{2}}}\pi ({{R}^{2}}-{{y}^{2}})dy$
$C{{M}_{y}}=\dfrac{1}{M}\int\limits_{0}^{M}{ydm}=\dfrac{1}{M}\int\limits_{0}^{R}{y}\dfrac{3M}{2{{R}^{3}}}\left( {{R}^{2}}-{{y}^{2}} \right)dy$
$C{{M}_{y}}=\dfrac{3}{2{{R}^{3}}}\int\limits_{0}^{R}{(y{{R}^{2}}-{{y}^{3}})}dy$
$C{{M}_{y}}=\dfrac{3R}{8}$
For the CM of a hemispherical shell, let us assume that the hemispherical shell is kept in the region $y>0$. Let us consider a ring contained at the periphery of the shell at height $y$, radius $r$ and subtends and $d\theta$ at the origin, $\theta$ is the angle at which the ring is considered from the x-axis. Therefore, the thickness of the ring is $Rd\theta$. Let the mass of this ring be $dm$ .
Let $dA$ be the surface area of the ring.
$dA=2\pi rRd\theta $
From trigonometry, it can be easily proved that $r=R\cos \theta $ and $y=R\sin \theta $ .
$\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:
$\dfrac{M}{A}=\dfrac{M}{2\pi {{R}^{2}}}$
$dm=\dfrac{M}{2\pi {{R}^{2}}}2\pi {{R}^{2}}\cos \theta d\theta =M\cos \theta d\theta $
$C{{M}_{y}}=\dfrac{1}{M}\int\limits_{0}^{M}{ydm}=\dfrac{1}{M}\int\limits_{0}^{\dfrac{\pi }{2}}{R\sin \theta M\cos \theta d\theta }$
$C{{M}_{y}}=\dfrac{R}{2}\int\limits_{0}^{\dfrac{\pi }{2}}{\sin (2\theta )d\theta }$
$C{{M}_{y}}=\dfrac{R}{2}$
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.
Recently Updated Pages
Four persons A B C and D initially at the corners of class 11 physics JEE_Main

What is the difference between Conduction and conv class 11 physics JEE_Main

Moment of inertia of solid sphere about its diameter class 11 physics JEE_Main

If a piece of ice floating on the surface of water class 11 physics JEE_Main

At what temperature speed of sound in air will be doubled class 11 physics JEE_Main

A closed organ pipe and an open organ pipe are tuned class 11 physics JEE_Main

Trending doubts
JEE Main 2026: Exam Dates, Session 2 Updates, City Slip, Admit Card & Latest News

Understanding the Electric Field of a Uniformly Charged Ring

Understanding Atomic Structure for Beginners

Electron Gain Enthalpy and Electron Affinity Explained

Derivation of Equation of Trajectory Explained for Students

How to Convert a Galvanometer into an Ammeter or Voltmeter

Other Pages
CBSE Notes Class 11 Physics Chapter 1 - Units And Measurements - 2026-27 PDF Download (Login Required)

NCERT Solutions For Class 11 Physics Chapter 1 Units And Measurements - 2026-27 Free PDF Download (Login Required)

NCERT Solutions For Class 11 Physics Chapter 2 Motion In A Straight Line - 2026-27 Free PDF Download (Login Required)

Important Questions For Class 11 Physics Chapter 1 Units and Measurement - 2026-27 Free PDF Download (Sign-in Required)

JEE Advanced Percentile vs Marks 2026: JEE Main Cutoff, AIR & IIT Admission Guide

CBSE Notes Class 11 Physics Chapter 2 - Motion in a Straight Line - 2026-27 PDF Download (Login Required)

