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A set of short answer and numerical questions related to rotational dynamics in physics. It includes detailed solutions for each question, covering concepts such as angular momentum, moment of inertia, and torque. The material is suitable for high school students studying physics, offering practical problems and step-by-step explanations to enhance understanding of rotational motion and its applications. The document also includes exercises for self-study, promoting active learning and problem-solving skills.
Typology: Cheat Sheet
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The angular momentum of the body moving in circular motion relative to the center of the circular path is always constant. i.e., | L~C | = |~r × p~| = mvrsinθ and since, r and v are perpendicular to each other.
Lc = mvr = mr^2 ω ∵ v = rω But relative to any other point except the center, the angular momentum is changing. Let us consider a point Q as in figure. In this case, the angular momentum is changing because r and θ changes throughout the motion. It can also be dealt in another way Since, r and F(centripetal force) are directed in opposite direction, then, τ = ~r × F~ = 0 relative to C and since, dL dtC = τ = 0. This implies, Lc= constant. But relative to any point (say, Q), LQ 6 = constant since ~r and F~ are oriented in different direction throughout the motion.
angular momentum is conserved.
i.e., L = Iω As I increases, the angular velocity(ω) of earth decreases to conserve the angular momentum. Since, ω = (^2) Tπ , the time period of rotation of earth then increases resulting in the increase in length of day.
L = Iω
As the ballet dancer stretches her hand, the moment of inertia (I = mr^2 : r is the distance from the axis of rotation) increases and thus the angular velocity of her should decrease to conserve the angular momentum. Due to this reason, ballet dancer stretches her hands to come to rest.
gsinθ K^2 R^2 + 1
Here, I=MK^2
compared to hard boiled egg. Hence, by watching the speed and time of egg to reach the bottom of the inclined plane, experienced cooks can distinguish raw eggs and hard boiled eggs.
initial revolution per second, f 0 = 50060 = 253 rev/sec final revolution per second, f = 20060 = 103 rev/sec angular acceleration, α=? time, t=4 sec
Now, ω = ω 0 + αt 2 πf = 2πf 0 + α × 4
2 π ×
= 2π ×
2 π
= 4α
4 α = − 10 π
α =
− 10 π 4 ∴ α = − 2. 5 π rad/s^2
The angular displacement is,
θ =
ω^2 − ω 02 2 α
=
(2π × 103 )^2 − (2π × 253 )^2 − 2 × 2. 5 π ∴ θ = 146. 61 rad ∵ θ = 2π × n , where n is the number of revolutions. Then, n =
θ 2 π
= 23. 33 rev
torque, τ = 500 Nm moment of inertia, I= 20 kgm^2 angular velocity, ω=? Kinetic energy gained, K.E.=? time, t= 2 s initial angular velocity, ω 0 = 0
Now, τ = Iα
α =
τ I ∴ α = 25 rad/s^2
angular velocity is, ω = ω 0 + αt = 25 × 2 ∴ ω = 50 rad/s
Then, the kinetic energy gained is,
K.E. =
Iω^2
=
2 π = ω 0 t +
αt^2
2 π =
αt^2 ∵ ω 0 = 0
4 π = αt^2
For the second revolution, i.e., n=2,
4 π =
α(t + 0.750)^2
From these two expressions,
αt^2 =
α(t + 0.750)^2
2 t^2 = t^2 + 2 × t × 0 .750 + (0.750)^2 t^2 − 1. 5 t − 0 .5625 = 0
When the frictional torque is applied, ω = 0,
α =
ω − ω 0 t′
=
rad/s^2
Thus, the frictional torque is,
τ ′^ = Iα
= 60 ×
∴ τ ′^ = 1 Nm
moment of inertia, I= 0.1 kgm^2 radius, r= 0.2 m angle of inclination, θ = 30◦ distance travelled by disc, s= 2 m mass of disc, m= 5 kg angular velocity, ω=?
When the disc rolls down a inclined plane,
loss in P.E. = mgh = mgssinθ
Total kinetic energy gained is,
mv^2 +
Iω^2
=
mω^2 r^2 +
Iω^2
=
ω^2 (mr^2 + I)
From these two equations,
loss in P.E. = gain in K.E.
mgssinθ =
ω^2 (mr^2 + I)
5 × 10 × 2 × sin 30 ◦^ =
ω^2 [5 × 0. 22 + 0.1]
50 =
ω^2 × 0. 3
ω^2 =
ω =
∴ ω = 18.25 rad/s
r =
d 2
= 0. 6 × 10 −^10 m
molecular speed of oxygen, v= 460m/s angular velocity, ω=?
Given, rotational kinetic energy (Erot) is two-thirds of translational kinetic