Moment Of Inertia Of A Ring

Moment Of Inertia Of A Ring

Edited By Vishal kumar | Updated on Jul 02, 2025 06:25 PM IST

The moment of inertia of a rigid body about a given axis of rotation is the sum of the products of the masses of the various particles and squares of their perpendicular distance from the axis of rotation. Two theorems, namely the perpendicular axis theorem and the parallel axis theorem, can be used to calculate the mass moment of inertia of a circular ring from the axis of rotation placed in the ring's plane, similar to a diameter passing from the centre, after determining the mass moment of inertia of the circular ring when the axis of rotation is passing from the centre.

Moment Of Inertia Of A Ring
Moment Of Inertia Of A Ring

In this article, we will cover the concept of the moment of inertia of a ring. This topic falls under the broader category of rotational motion, which is a crucial chapter in Class 11 physics. It is not only essential for board exams but also for competitive exams like the Joint Entrance Examination (JEE Main), National Eligibility Entrance Test (NEET), and other entrance exams such as SRMJEE, BITSAT, WBJEE, BCECE and more. Over the last ten years of the JEE Main exam (from 2013 to 2023), three questions have been asked on this concept. And for NEET one question was asked from this concept.

Let's read this entire article to gain an in-depth understanding of the moment of inertia of a ring

Moment of Inertia of a Ring

Let I= Moment of inertia of a RING about an axis through its centre and perpendicular to its plane.

To find out I Consider a ring of mass m, radius R and centre O.

Take an elementary portion of the ring of mass dm and length dx.

dm=(m/2πR)dx

Next, we calculate dl=(dm)R2
dl=[(m/2πR)dx]R2

Substituting the values, we get;
dl=(m/2πR)R2dx

Using integration;
I=(mR/2π)J2πRdxI=(m/2π)[x]002πRI=(mR/2π)[2πR0]I=mR2

Moment of Inertia of a Ring About an Axis Passing Through Its Diameter

From the formula, which we study earlier;
I=r2dm

Now, We need to find dm. We will get;
dm=M/2πdθ

Meanwhile, r=rcosθ
The next step is to carry out the integration. We will have;
I=o2πr2cos2θ(M/2π)dθI=Mr2/2π2πcos2θdθI=Mr2/2π[θ/2+sin2θ/4]Io2πI=Mr2/2π[(π+0)(0+0)]I=Mr2/2

Following this derivation, we'll go on to several solved examples to help you understand the concept.



Solved Examples Based on the Moment of Inertia of a Ring

Example 1: The moment of inertia of a circular wire of mass M and radius R about its diameter is

1) MR2/2
2) MR2
3) 2MR2
4) MR2/4

Solution:

Moment of inertia for Ring -
I=MR2
wherein
About an axis perpendicular to the ring \& passing through the centre.
The moment of inertia of a circular wire about a diameter is 12MR2
I=12MR2

Hence, the answer is the option (1).

Example 2: Moment of inertia of a semi-circular ring about an axis which is perpendicular to the plane of the ring and passes through the centre :

1) MR2
2) 2MR2
3) MR22
4) MR24

Solution:

Moment of inertia for Ring
Let I= the Moment of inertia of a ring of mass m about an axis through its centre and perpendicular to its plan- I=mR2

Consider a whole ring of mass m=2M, radius R, and centre O.
I=(2M)R2

For half ring

Therefore the half portion of the Ring will be a semicircular ring of Radius (R) and mass (M)

$\Rightarrow$The moment of Inertia of the semicircular Ring will also be halved

I=I2=(2M)R22I=MR2Hence,theanswerisoption(1)

Example 3: What will be the moment of inertia of a ring whose mass is not uniformly distributed? Given that the density of the material is ρ and the radius is R, the total mass of the ring is M.

1) MR22
2) MR2
3) MR2ρ
4) MR22ρ

Solution:

The moment of inertia in both the cases i.e., when mass is uniformly distributed or non-uniformly distributed is the same. Because dm=M is the same in both cases. So, the answer will be MR2

Hence, the answer is the option 2.

Example 4: Two rings have their moment of inertia in the ratio of 2:1 and their diameter are in the ratio 1:2. The ratio of the masses of the rings will be:

1) 4:1

2) 2:1

3) 1:4

4) 8:1

Solution:

I1I2=M1R12M2R2221=M1M2×14M1M2=81

Hence, the answer is the option (4).

Example 5: The moment of inertia of a uniform thin rod about a perpendicular axis passing through one end is I1. The same rod is bent into a ring and its moment of inertia about a diameter is I2. If I1I2 is xπ23, then the value of x will be .

1) 8

2) 16

3) 24

4) 56

Solution:

2πR=lI=mR22=m2×l24π2=ml28π2I1I2=ml2/3ml2/8π2=8π23x=8

Hence the answer is (8).

Summary

The moment of inertia for a rigid body is a physical quantity that combines mass and shape in Newton's equations of motion, momentum, and kinetic energy. The moment of inertia is applied in both linear and angular moments, although it manifests itself in planar and spatial movement in rather different ways. One scalar quantity defines the moment of inertia in planar motion.

Frequently Asked Questions (FAQs):

Q 1: What is the formula for the moment of inertia of a ring?

Ans: The formula for the moment of inertia of a rod when the axis is through the centre is $I = MR^2.$

Q 2: What is a circular ring?

Ans: A circular ring is an equal mass distribution system of particles where the particles are placed at an equal distance from the centre.

Q 3: Is there any difference between the moment of inertia and rotational inertia?

Ans: No

Q 4: Is the moment of inertia a scalar or a vector quantity?

Ans: Scalar quantity

Q 5: Does the moment of inertia change with the change of the axis of rotation?

Ans: Yes

Frequently Asked Questions (FAQs)

1. What is the moment of inertia of a ring?
The moment of inertia of a ring is a measure of its resistance to rotational acceleration. For a ring with mass M and radius R, the moment of inertia is given by I = MR^2. This means all the mass is concentrated at a distance R from the axis of rotation, making it more resistant to changes in rotational motion compared to objects with mass distributed closer to the axis.
2. How does the moment of inertia of a ring compare to that of a solid disk of the same mass and radius?
The moment of inertia of a ring (I = MR^2) is greater than that of a solid disk (I = 1/2 MR^2) with the same mass and radius. This is because all of the ring's mass is concentrated at its outer edge, while the disk's mass is distributed throughout its area. As a result, the ring is more resistant to changes in rotational motion.
3. Why is the moment of inertia of a ring important in real-world applications?
The moment of inertia of a ring is important in various applications because it affects rotational dynamics. For example, in flywheels used in engines or exercise equipment, a higher moment of inertia (like that of a ring) helps maintain steady rotation and store rotational energy more effectively. This property is also crucial in the design of gyroscopes, where maintaining angular momentum is essential.
4. How does changing the radius of a ring affect its moment of inertia?
The moment of inertia of a ring is proportional to the square of its radius (I = MR^2). This means that doubling the radius will quadruple the moment of inertia, while halving the radius will reduce the moment of inertia to one-fourth of its original value. This relationship demonstrates why even small changes in radius can significantly impact a ring's rotational behavior.
5. What happens to the moment of inertia if you distribute the ring's mass evenly throughout its area instead of concentrating it at the edge?
If you distribute the ring's mass evenly throughout its area, effectively turning it into a disk, the moment of inertia would decrease. The formula would change from I = MR^2 for a ring to I = 1/2 MR^2 for a disk. This reduction occurs because some of the mass is now closer to the axis of rotation, making the object less resistant to rotational acceleration.
6. How does the moment of inertia of a ring relate to its angular momentum?
The moment of inertia of a ring is directly related to its angular momentum. Angular momentum (L) is the product of moment of inertia (I) and angular velocity (ω): L = Iω. For a given angular velocity, a ring with a larger moment of inertia will have greater angular momentum. This relationship is crucial in understanding the rotational dynamics of ring-shaped objects.
7. Can the moment of inertia of a ring be changed without altering its mass or radius?
The moment of inertia of a perfect, uniform ring cannot be changed without altering its mass or radius, as it is defined by the formula I = MR^2. However, in practical applications, you can affect the effective moment of inertia by adding or removing mass at different radii, or by changing the ring's shape slightly (e.g., making it slightly thicker or thinner at different points).
8. How does the rotational kinetic energy of a ring relate to its moment of inertia?
The rotational kinetic energy of a ring is directly proportional to its moment of inertia. The formula for rotational kinetic energy is KE = 1/2 Iω^2, where I is the moment of inertia and ω is the angular velocity. A ring with a larger moment of inertia will have more rotational kinetic energy for a given angular velocity compared to an object with a smaller moment of inertia rotating at the same speed.
9. Why is the moment of inertia of a ring larger than that of a point mass at the same radius?
The moment of inertia of a ring (I = MR^2) is larger than that of a point mass (I = MR^2) at the same radius because the ring has its mass distributed around its circumference. Although the formulas appear identical, the ring's structure makes it inherently more resistant to changes in rotational motion. This is due to the ring's mass being spread out, requiring more torque to change its rotational state compared to a point mass.
10. How does the moment of inertia of a ring affect its angular acceleration when a torque is applied?
The moment of inertia of a ring inversely affects its angular acceleration when a torque is applied. According to the rotational form of Newton's Second Law, τ = Iα, where τ is torque, I is moment of inertia, and α is angular acceleration. For a given torque, a ring with a larger moment of inertia will experience less angular acceleration compared to an object with a smaller moment of inertia.
11. What is the significance of the parallel axis theorem in relation to a ring's moment of inertia?
The parallel axis theorem is significant for calculating a ring's moment of inertia about any axis parallel to its central axis. It states that the moment of inertia about a parallel axis is equal to the moment of inertia about the center of mass plus the product of the mass and the square of the perpendicular distance between the axes. This theorem is crucial for analyzing the rotational dynamics of rings in various orientations.
12. How does the thickness of a ring affect its moment of inertia?
For an ideal, infinitely thin ring, the thickness doesn't affect the moment of inertia. However, for real rings with finite thickness, increasing the thickness while maintaining the same outer radius and mass will slightly decrease the moment of inertia. This is because some mass is distributed closer to the axis of rotation. The effect is usually small for thin rings but becomes more significant as the ring approaches a cylindrical shape.
13. Why is the moment of inertia of a ring important in the design of gyroscopes?
The moment of inertia of a ring is crucial in gyroscope design because it directly affects the gyroscope's ability to maintain its orientation. A larger moment of inertia, characteristic of a ring, provides greater resistance to changes in angular momentum. This property allows gyroscopes to maintain their axis of rotation more steadily, making them more effective for navigation, stabilization, and measurement applications.
14. How does the moment of inertia of a ring compare to that of a hollow cylinder of the same mass and radius?
The moment of inertia of a ring (I = MR^2) is slightly larger than that of a hollow cylinder of the same mass and radius. For a hollow cylinder, the moment of inertia is I = M(R1^2 + R2^2)/2, where R1 and R2 are the outer and inner radii. As the wall thickness of the cylinder approaches zero (R1 ≈ R2), its moment of inertia approaches that of a ring. The ring's slightly higher moment of inertia is due to all its mass being at the maximum radius.
15. Can you explain why the moment of inertia of a ring is independent of its width (along the axis of rotation)?
The moment of inertia of an ideal ring is independent of its width along the axis of rotation because all the mass is considered to be concentrated at a single radius. The formula I = MR^2 only considers the mass and the distance from the axis of rotation. The width doesn't affect these parameters, so it doesn't influence the moment of inertia. This is an idealization, and for very wide rings, the distribution of mass along the width would start to have a small effect.
16. How does the rotational period of a ring relate to its moment of inertia?
The rotational period of a ring is related to its moment of inertia through the concept of angular velocity. For a given angular momentum, a ring with a larger moment of inertia will have a slower angular velocity (ω = L/I, where L is angular momentum). Since the period (T) is inversely proportional to angular velocity (T = 2π/ω), a larger moment of inertia results in a longer rotational period, assuming constant angular momentum.
17. What role does the moment of inertia of a ring play in the concept of precession?
The moment of inertia of a ring plays a crucial role in precession, which is the change in the orientation of the rotational axis. A ring's large moment of inertia resists changes to its angular momentum vector. When an external torque is applied perpendicular to the spin axis, instead of toppling, the ring's axis of rotation slowly traces out a cone shape. The rate of precession is inversely proportional to the moment of inertia, so rings with larger moments of inertia precess more slowly.
18. How does the concept of moment of inertia of a ring apply to planetary rings, like those of Saturn?
The concept of moment of inertia applies to planetary rings like Saturn's in that it helps explain their rotational dynamics. Although planetary rings are composed of many individual particles, they can be modeled as a collection of concentric rings, each with its own moment of inertia. This collective moment of inertia affects how the ring system responds to gravitational perturbations from moons and contributes to the overall angular momentum of the Saturn system.
19. Why is the moment of inertia of a ring important in the design of certain types of motors and generators?
The moment of inertia of a ring is important in the design of certain motors and generators because it affects the rotational dynamics of these machines. A larger moment of inertia, like that of a ring, can help maintain steady rotation and reduce fluctuations in angular velocity. This is particularly useful in flywheel energy storage systems, where the high moment of inertia of a ring-like structure allows for efficient storage and release of rotational energy.
20. How does the moment of inertia of a ring affect its behavior when rolling down an inclined plane?
The moment of inertia of a ring significantly affects its behavior when rolling down an inclined plane. Compared to a solid disk of the same mass and radius, a ring will roll down more slowly. This is because a larger fraction of the ring's kinetic energy is in rotational form due to its higher moment of inertia. The linear acceleration of a rolling ring is given by a = g sin(θ) / (1 + I/MR^2), where θ is the incline angle. For a ring, I/MR^2 = 1, resulting in slower acceleration compared to objects with smaller moments of inertia.
21. What is the relationship between the moment of inertia of a ring and its radius of gyration?
The radius of gyration (k) is related to the moment of inertia (I) and mass (M) of a ring by the equation I = Mk^2. For a ring rotating about its central axis, the radius of gyration is equal to its physical radius (R). This means that for a ring, k = R, and the moment of inertia can be expressed as I = MR^2. The radius of gyration represents the distance from the axis of rotation at which all the mass could be concentrated to give the same moment of inertia.
22. How does adding mass to the inner edge of a ring affect its moment of inertia?
Adding mass to the inner edge of a ring decreases its overall moment of inertia relative to its total mass. While the added mass contributes to the moment of inertia, it does so less than if it were added to the outer edge. This is because the moment of inertia depends on the square of the distance from the axis of rotation (I = Σmr^2). Mass closer to the center has less impact, so the average moment of inertia per unit mass decreases, making the ring slightly easier to rotate for its new total mass.
23. Can you explain how the moment of inertia of a ring relates to its angular momentum conservation?
The moment of inertia of a ring is crucial in understanding its angular momentum conservation. Angular momentum (L) is the product of moment of inertia (I) and angular velocity (ω): L = Iω. When no external torque is applied, angular momentum is conserved. If the ring's moment of inertia changes (e.g., by changing its radius), its angular velocity must change inversely to maintain constant angular momentum. This principle is why figure skaters spin faster when they pull their arms in, effectively reducing their moment of inertia.
24. How does the moment of inertia of a ring affect its stability when rotating about its diameter?
When a ring rotates about its diameter (an axis perpendicular to its normal axis of symmetry), its moment of inertia is half of what it is when rotating about its central axis: I = 1/2 MR^2. This smaller moment of inertia makes the ring less stable in this orientation. It's more susceptible to wobbling and precession, as less energy is required to change its axis of rotation. This instability is why a rolling hoop is less stable than a disk rolling on its edge.
25. What is the significance of the moment of inertia of a ring in the context of rotational equilibrium?
The moment of inertia of a ring is significant in rotational equilibrium because it determines how the ring responds to torques. In equilibrium, the net torque on the ring must be zero. The ring's large moment of inertia means it strongly resists changes to its rotational state. This resistance helps maintain equilibrium against small perturbations, making rings (or ring-like structures) useful in applications where rotational stability is important, such as in certain types of balances or in the design of stable rotating platforms.
26. How does the moment of inertia of a ring affect its rotational energy distribution in a collision?
The moment of inertia of a ring significantly affects its rotational energy distribution in a collision. Due to its high moment of inertia (I = MR^2), a larger proportion of the ring's kinetic energy is in rotational form compared to objects with lower moments of inertia. In a collision, this means that more energy is likely to be transferred into or out of rotational motion. The ring's behavior during and after the collision will be notably different from that of a solid disk or sphere, potentially resulting in less linear velocity change and more rotational effects.
27. Why is understanding the moment of inertia of a ring important in analyzing the motion of hula hoops?
Understanding the moment of inertia of a ring is crucial in analyzing hula hoop motion because it explains the hoop's resistance to changes in its rotational state. The large moment of inertia of a hula hoop (approximated as a ring) allows it to maintain its plane of rotation even as the user's hips move. This resistance to change, combined with the torque applied by the user, creates the characteristic wobbling motion. The hoop's high moment of inertia also explains why it's easier to keep a larger hoop rotating compared to a smaller one of the same mass.
28. How does the moment of inertia of a ring compare to that of a thin rod of the same mass and length?
The moment of inertia of a ring (I = MR^2) is significantly larger than that of a thin rod of the same mass and length rotating about its center. For a rod, the moment of inertia about its center is I = 1/12 ML^2, where L is its length. If we consider the rod's length equal to the ring's diameter, the ring's moment of inertia is 4 times greater than the rod's. This difference illustrates why ring-shaped objects are more resistant to changes in rotational motion compared to rod-shaped objects of similar dimensions.
29. What is the importance of the moment of inertia of a ring in the design of certain types of pendulums?
The moment of inertia of a ring is important in the design of certain pendulums, particularly in precision timekeeping devices. Ring-shaped bobs in pendulums, due to their high moment of inertia relative to their mass, are less affected by small variations in air resistance or other perturbations. This property helps maintain consistent oscillations. Additionally, the well-defined moment of inertia of a ring makes it easier to calculate and adjust the pendulum's period accurately, which is crucial for precise timekeeping.
30. How does the concept of moment of inertia of a ring apply to the design of bicycle wheels?
The concept of moment of inertia of a ring applies significantly to bicycle wheel design. Bicycle wheels, with most of their mass concentrated in the rim and tire, approximate a ring in terms of moment of inertia. This high moment of inertia contributes to the wheel's gyroscopic effect, enhancing stability while riding. It also helps maintain steady motion, as the wheels resist changes in rotational speed. However, designers must balance this with the need for lightweight wheels, as a higher moment of inertia also means more energy is required to accelerate or decelerate the bicycle.
31. Why is the moment of inertia of a ring relevant in understanding the behavior of rotating space stations?
The moment of inertia of a ring is relevant to rotating space stations because many designs propose a ring-like structure to create artificial gravity through centripetal acceleration. The high moment of inertia of a ring-shaped station would provide rot

Articles

Back to top