x = a + b t 2 + c t 3 x = a+bt^2+ct^3 x = a + b t 2 + c t 3
The angular velocity of rotation is a vector numerically equal to the first derivative \text{The angular velocity of rotation is a vector numerically equal to the first derivative} The angular velocity of rotation is a vector numerically equal to the first derivative
of the angle of rotation of the body \text{of the angle of rotation of the body} of the angle of rotation of the body
ω ⃗ = x ′ = 2 b t + 3 c t 2 \vec\omega= x'=2bt+3ct^2 ω = x ′ = 2 b t + 3 c t 2
Angular acceleration is a vector quantity equal to the first derivative \text{Angular acceleration is a vector quantity equal to the first derivative} Angular acceleration is a vector quantity equal to the first derivative
of the angular velocity with respect to time \text{{of the angular velocity with respect to time}} of the angular velocity with respect to time
α ⃗ = ω ⃗ ′ = 2 b + 6 c t \vec\alpha=\vec\omega'=2b+6ct α = ω ′ = 2 b + 6 c t
Answer : ω ⃗ = 2 b t + 3 c t 2 ; α ⃗ = 2 b + 6 c t \text{Answer : }\vec\omega= 2bt+3ct^2;\vec\alpha=2b+6ct Answer : ω = 2 b t + 3 c t 2 ; α = 2 b + 6 c t
Comments