Correct Answer - Option 1 : 10
Concept:
The equations which are applied in linear motion can also be applied in angular motion.
|
Linear Motion
|
Rotational Motion
|
|
Position
|
x
|
θ
|
Angular position
|
Velocity
|
v
|
ω
|
Angular velocity
|
Acceleration
|
a
|
α
|
Angular acceleration
|
Motion equations
|
x = v̅ t
|
θ = ω̅t
|
Motion equations
|
|
v = v0 + at
|
ω = ω0 + αt
|
|
|
\(x = {v_0}t + \frac{1}{2}a{t^2}\)
|
\(θ = {ω _0}t + \frac{1}{2}α {t^2}\)
|
|
|
\({v^2} = v_0^2 + 2ax\)
|
\({ω ^2} = ω _0^2 + 2α θ\)
|
|
Mass (linear inertia)
|
M
|
I
|
Moment of inertia
|
Newton’s second law
|
F = ma
|
τ = Iα
|
Newton’s second law
|
Momentum
|
p = mv
|
L = Iω
|
Angular momentum
|
Work
|
Fd
|
τθ
|
Work
|
Kinetic energy
|
\(\frac{1}{2}m{v^2}\)
|
\(\frac{1}{2}I{ω ^2}\)
|
Kinetic energy
|
Power
|
Fv
|
τω
|
Power
|
Calculation:
Given:
α = 3 rad/s2, ωo = 2 rad/s, t = 2 s
We know that,
\(θ = {ω _0}t + \frac{1}{2}α {t^2}\)
\(θ = ({2}\times 2) + \frac{1}{2}\times3\times2^2\)
θ = 4 + 6 = 10 radians