With JEE Main 2022 notification expected to be out in 3rd week of December, 2021, candidates aspiring to give the exam should ensure that they are well acquainted with the important topics. With JEE Main Study notes for Rotational dynamics, we have covered below important topics of rotational dynamics, previous year questions that will assist in your preparation for JEE Physics Syllabus. As per previous years analysis, Rotational Dynamics has a weightage of 6.67% in JEE Main Physics, with at least 2 questions expected in the exam. Check JEE Main Physics Syllabus
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Note- Centripetal and centrifugal force are opposite in direction but equal in magnitude. It is not to be confused as action and reaction because they act on two different bodies and not on the same.
Moment of Inertia for differently shaped bodies is given as below-
Type | Shape | Formula |
---|---|---|
Point Mass at Radius R | ||
Thin rod about an axis through center perpendicular to the length | ||
Thin rod about an axis through end perpendicular to the length | ||
Thin wall cylinder about the central axis | ||
Thick wall cylinder about the central axis | ||
Solid cylinder about the central axis | ||
Solid cylinder about the central diameter | ||
Solid sphere about the center | ||
Thin hollow sphere about the center | ||
Thin ring about the diameter | ||
Slab about the perpendicular axis through the center | ||
Cone about central axis |
Check Gujarat Board Released Question Banks for JEE Main
“It states that the Moment of Inertia of a planar body (lamina) about an axis perpendicular to its plane is equal to the sum of its moments of inertia about two perpendicular axes concurrent with perpendicular axis and lying in the plane of the body.”
The theorem is stated as “The Moment of Inertia of a body about any axis is equal to the sum of the Moment of Inertia of the body about a parallel axis passing through its center of mass and the product of its mass and the square of the distance between the two parallel axes”.
where Iz and Iz′ = the moments of Inertia of the body about the z and z ′ axes respectively
M = total mass of the body
a=perpendicular distance between the two parallel axes
p = magnitude of p and Ѳ = angle between r and p.
Where I=Moment of Inertia and M=mass of the body.
where,
M=mass of the body
vcm = rotational motion
I =moment of Inertia
ω =the angular velocity of the rolling body
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1] linear acceleration (a) and angular acceleration (α)
a] Scalar form is
a= rα
b] Vector form is
c] Tangential component is
d] Radial component is
2] linear acceleration (a), angular velocity (ω) and linear velocity (v)
a=v2/r = ω2/r
3] Inertia (I) and Torque (T)
4] Moment of Inertia (I) and Angular momentum (L)
Phenomenon |
Formula |
Elaboration |
---|---|---|
Equations of rotational kinematics |
ω=ω0+αt θ = ω0t + ½ αt2 ω2 – ω02 = 2αθ θnth = ω0 +α/2 (2n-1) |
Angular velocity after a time t second Angular displacement after t second Angular velocity after a certain rotation Angle traversed in ‘nth' second. |
Tangential Velocity |
V=2πr/time |
r = radius of the motion path T=period of the motion |
Angular Velocity |
ω=2π/T=2πf |
T= period of the motion f= frequency |
Angular/Centripetal Acceleration |
acentripetal = -4π²r/T² acentripetal = -ω2r acentripetal = v²/r |
ω = angular velocity r=radius and v =tangential velocity |
Centripetal Force |
Fc=-m4π²r/T² Fc=mv²/r |
T = period V=tangential velocity m= mass of the object |
Torque |
Τ=F.d.sinΘ |
F=Applied Force. D=Distance |
Moment of Inertia for a system of particles |
I = ∑mr2 |
I=Moment of Inertia, m=mass R=radius |
Moment of Inertia for rigid bodies |
I = ∫ r2 dm |
Dm= infinitesimal element of mass R=distance between the mass element and the axis of rotation |
Question: A circular disc of radius R and mass 9 M, a small disc of radius R/3 is removed as shown in the figure. Calculate the Moment of Inertia of the remaining disc about an axis perpendicular to the plane of the disc and passing through the center of the disc.
Solution-
The moment of Inertia of the removed part above the axis passing through the center of mass and perpendicular to the plane of the disc = Icm + md2
= [m × (R/3)2]/2 + m × [4R2/9] = mR2/2
Hence, the moment of Inertia of the remaining portion = moment of Inertia of the complete disc – the Moment of Inertia of the removed portion
= 9mR2/2 – mR2/2 = 8mR2/2
= 4mR2.
Question: Calculate the instantaneous power of a wheel rotating with an angular velocity of 20rad/s, when a torque of 10Nm is applied.
Solution- P=ꞇꞶ
=10 x20=200W.
Question: A cylinder of mass 5kg and radius 10 cm is moving on a horizontal surface with speed 5m/s and angular speed about the axis through CM 10 rad/s. What is the angular momentum of the cylinder about the point of contact?
Solution- LO =MVcm.r
=5x5x1/10
=2.5kg m2/s
Lcm=1/2 MR2
=1/2x5x [1/10]2 x 10
= ¼ or 0.25 kgm2/s
Therefore, L=Lo + Lcm=2.5 +0.25=2.75 kgm2/s.
*The article might have information for the previous academic years, please refer the official website of the exam.