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Fixed axis rotation of rigid body

Fixed axis rotation of rigid body
There is a straight line of motionless movement in the rigid body, called rotation for short. This fixed line is called the rotation axis of the rigid body. Obviously, other points in the rigid body move in circles in planes perpendicular to the rotation axis, with the center on the rotation axis.
Chinese name
Fixed axis rotation of rigid body
Foreign name
rotation of a rigid body about a fixed axis

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Any point in the rigid body Q And its circumferential trajectory center O ''s connection O ' Q (Figure 1) is called the turning radius of the point. From fixed plane Ozx Angle to rotation plane OzQ φ , which can be used to determine the instantaneous position of the rigid body. corner φ Over time t The change law of is called the rotation equation of rigid body. Write:
φ=f t
corner φ Change Δ of φ And corresponding time interval Δ t Ratio Δ of φ/ Δ t=ω* It is called average angular velocity. When Δ t → 0, ω *Limit of trend ω Is called (instantaneous) angular velocity, i.e
Current angular velocity ω Over time t When changing, its change Δ ω And corresponding time interval Δ t Ratio Δ of ω/ Δ t=ε* It is called average angular acceleration. When Δ t → 0, ε *Limit of trend ε Is called (instantaneous) angular acceleration, namely
The angular velocity and angular acceleration of a rigid body can be expressed along the axis of rotation Oz (Unit vector is k )The slip vector of. (Figure 2). Angular velocity vector ω And angular acceleration vector ε Can write separately ω = ωk ε = εk
Rotate any point in the rigid body Q Linear speed of v be equal to v = ω × r , and v = ω · O´Q spot Q Linear acceleration of α For:
α = α t + α n = ε × r + ω × v
And α t = ε · O´Q α n = ω · O´Q
In the above formula r Any point on the shaft O To point Q Vector diameter of, and α t and α n Points respectively Q Tangential and normal acceleration of (see acceleration).
The magnitude of the rigid body's moment of inertia is related to the following factors:
(1) Rigid bodies with the same shape and size have large mass and large moment of inertia;
(2) For rigid bodies with the same total mass, the farther the mass distribution is away from the axis, the greater the moment of inertia;
(3) For the same rigid body, if the rotation axis is different, the distribution of the mass to the axis is different, and the size of the moment of inertia is different.