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Rotational motion
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Physics, Class 11, Chapter 7
System of Particles
and Rotational Motion
For IIT JEE, NEET, Boards & Olympiad | Made with love by Vikrant Kirar
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Rigid Body
A body with perfectly definite and unchanging shape.
The distance between two points of a rigid body does
not change.
रिजिड बॉडी के ककन्ही भी दो पॉइंट्स के बीच की दूिी बदलती नहीं है।
इसके जलए वह इंटिनल फोसेि का इस्तेमाल किती है।
Types of Motion
Translational Motion
Every point on the body has same velocity. No
rotation.
बॉडी के पॉइंट्स की वेलोजसटी बिाबि होती है।
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Circular Motion
Circular path, but no rotation. Mostly meant for point
objects.
िोटेशन नहीं होता है। चाय कप से गििेिी नहीं।
Rotational Motion
Circular Motion with rotation of body.
बॉडी िोटेट भी कि िही है। चाय गिि िाएिी।
Combination
Rotation and translation together.
Examples
Pure rotation: Fan
Pure translation: Wagon of a train
Pure rolling: Wheel of a train
Pure circular motion: difficult to find in nature
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Overview
Translational Angular
Position Angular Position
Displacement Angular Displacement
Velocity Angular Velocity
Acceleration Angular acceleration
Mass (inertia) Moment of Inertia
Momentum Angular Momentum
Force Torque
Kinetic Energy Rotational Kinetic Energy
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Right-Hand Rule
All angular quantities have
magnitude and direction. But
they are not vector.
A + B ≠ B + A.
is not vector.
& are pseudo vectors.
We will only study rotation about a fixed axis. For fixed
axis of rotation, we can treat them as vectors.
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Linear and Angular Motion
We’re interested in distance, not displacement.
Distance = arc length =
Angular Velocity
Angular Acceleration (Tangential)
Centripetal Acceleration (Radial) भूलना मत
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Frequency
How many times per second (or per day/minute)
SI Unit: Hz (hertz).
1 Hz = 1 per second.
Time Period
Frequency = f
Time Period = T
T = 1/f
One Revolution
2π radian = 1 revolution
𝜔 = 2𝜋𝑓
𝑇 =
2 𝜋
𝜔
=
1
𝑓
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Moment of Inertia
Resistance to rotate. Inertia to rotate.
Depends upon mass and its distribution.
मास एक्लिस से जितना दूि होिा, उसे घूमना उतना ही मुश्किल होिा।
Discrete Mass Distribution
Continuous Mass Distribution
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Rigid Body Dynamics
Every particle of the
body moves in a circle
which lies in a plane
perpendicular to the
axis and has its center
on the axis.
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Center of Mass
CoM moves as if all the mass of the system was
concentrated at CoM and all external forces were
applied at that point.
F=Ma
Other parts may feel some different forces due to
internal forces.
Center of Gravity
Point where the total gravitational torque on the body
is zero. For Uniform gravitational field, it’s same as
CoM.
CoG = CoM CoG = CoM
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Equilibrium of a Rigid Body
The linear and angular momentum must be constant.
For mechanical equilibrium, net force and net torque
should be zero.
Examples of a rod not in equilibrium.
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Topple
If friction is sufficient, the body may rotate before
translation starts.
सिकने से पहले लुढ़क िाती है।
The normal reaction shifts to avoid topple.
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Couple
A pair of equal and opposite forces with different lines
of action is known as a couple.
Net force is zero. CoM does not move.
It does not matter where you apply the force, Torque
is always the same.
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Kinetic Energy
Total KE = Rotational KE + Translational KE
For Hinged motion, using the parallel axes theorem,
the above formula becomes
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Translation to Rolling
िब तक pure rolling शुरू नहीं होती, तब तक acceleration औि
angular acceleration constant िहेंिे। क्योंकक अभी pure rolling
नहीं हो िही है, Instantaneous Axis of Rotation का इस्तेमाल नहीं
कि सकते।
मान लो pure rolling शुरू होने में समय लिा 't'
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Rolling to Translation
िब तक pure rolling शुरू नहीं होती, तब तक acceleration औि
angular acceleration constant िहेंिे। क्योंकक अभी pure rolling
नहीं हो िही है, Instantaneous Axis of Rotation का इस्तेमाल नहीं
कि सकते।
मान लो pure rolling शुरू होने में समय लिा 't'
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Pure Rolling on an Incline
Pure rolling हो िही है, इसीजलए Instantaneous Axis of
Rotation इस्तेमाल ककया िा सकता है।