vector. Further, the angular acceleration, α =
Chapter 6: SYSTEMS OF PARTICLES AND ROTATIONAL MOTION · PHYSICS · EN medium
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d ω /d t . The kinematical quantities in rotational motion, angular displacement ( θ ), angular velocity ( ω ) and angular acceleration ( α ) respectively are analogous to kinematic quantities in linear motion, displacement ( x ), velocity ( v ) and acceleration ( a ). We know the kinematical equations of linear motion with uniform (i.e. constant) acceleration: v = v + at (a) at υ (b) ax υ υ (c) where x = initial displacement and v = initial velocity. The word ‘initial’ refers to values of the quantities at t = The corresponding kinematic equations for rotational motion with uniform angular acceleration are: ( . ) ( . ) and ( – α θ ( .
📖 ncert books class 11 physics chapter 6 · Page 26
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d ω /d t . The kinematical quantities in rotational motion, angular displacement ( θ ), angular velocity ( ω ) and angular acceleration ( α ) respectively are analogous to kinematic quantities in linear motion, displacement ( x ), velocity ( v ) and acceleration ( a ). We know the kinematical equations of linear motion with uniform (i.e. constant) acceleration: v = v + at (a) at υ (b) ax υ υ (c) where x = initial displacement and v = initial velocity.
The word ‘initial’ refers to values of the quantities at t = The corresponding kinematic equations for rotational motion with uniform angular acceleration are: ( . ) ( . ) and ( – α θ ( . ) where θ = initial angular displacement of the rotating body, and ω = initial angular velocity of the body.
Fig. . Specifying the angular position of a rigid body.
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