10.11
Teorema do Eixo Paralelo
O teorema do eixo paralelo fornece um método conveniente e rápido de encontrar o momento de inércia de um objeto em relação a um eixo paralelo ao eixo…
Pode haver vários eixos possíveis ao longo dos quais um corpo rígido pode girar e, portanto, correspondentemente, pode haver vários momentos de inércia para o mesmo corpo.
Se o momento de inércia, ICM , em torno de um eixo que passa pelo centro de massa é conhecido, então o momento de inércia em torno de qualquer outro eixo paralelo pode ser obtido usando o teorema do eixo paralelo.
O teorema afirma que o momento de inércia ao longo de qualquer eixo paralelo ao eixo que passa pelo centro de massa é dado como a soma de ICM e o produto da massa do corpo e o quadrado da distância perpendicular entre os dois eixos.
Considere uma porta de massa M e altura 2L. A largura da porta é metade da altura da porta. A porta gira em torno de suas dobradiças.
O ICM da porta é igual a ML2 por doze. O momento de inércia ao longo do eixo de rotação é assim dado como a soma de ICM e ML2 por quatro.
View the full transcript and gain access to JoVE Core videos
Q1: What is the parallel-axis theorem and why is it useful?
The parallel-axis theorem states that the moment of inertia about any axis parallel to an axis through the center of mass equals the moment of inertia through the center of mass plus the product of mass and the square of the perpendicular distance between axes. This theorem provides a convenient method for calculating moments of inertia without lengthy integration, making it especially useful when the center-of-mass moment of inertia is already known.
Q2: How does the parallel-axis theorem apply to a rotating door?
For a door of mass M and height 2L rotating about its hinges, the moment of inertia is calculated using the parallel-axis theorem. Given that the center-of-mass moment of inertia is ML²/12, the total moment of inertia about the hinge axis equals ICM plus ML²/4, which accounts for the perpendicular distance between the hinge axis and the center of mass.
Q3: Why is the parallel-axis theorem more efficient than conventional integration methods?
The conventional method for finding moment of inertia requires linear mass density concepts and integration along an object's length, which is cumbersome and lengthy. The parallel-axis theorem bypasses this process by using a known center-of-mass moment of inertia and applying a simple distance correction, yielding identical results with significantly less calculation.
Q4: How does the perpendicular distance between axes affect moment of inertia calculations?
The perpendicular distance between the rotation axis and the center-of-mass axis is squared and multiplied by the body's mass in the parallel-axis theorem formula. This squared distance term means that even small increases in separation significantly increase the moment of inertia, reflecting how rotating objects farther from their center of mass requires more rotational resistance.
Q5: Can the parallel-axis theorem be applied to a thin rod rotating about its end?
Yes, the parallel-axis theorem simplifies finding the moment of inertia of a thin rod about an axis through its end. If the moment of inertia about the center of mass is known, the end-axis moment of inertia equals the center-of-mass value plus the product of mass and the square of half the rod's length, avoiding lengthy conventional calculations.
Q6: What is the mathematical formula for the parallel-axis theorem?
The parallel-axis theorem formula is I = ICM + Md², where I is the moment of inertia about the parallel axis, ICM is the moment of inertia through the center of mass, M is the body's mass, and d is the perpendicular distance between the two parallel axes. This relationship holds for any rigid body rotating about axes parallel to the center-of-mass axis.
Q7: How does the parallel-axis theorem relate to rotational motion analysis?
The parallel-axis theorem is fundamental to analyzing rotational motion because it allows quick calculation of moment of inertia for any parallel axis once the center-of-mass value is known. Understanding moment of inertia through this theorem is essential for studying moment of inertia and rotational kinetic energy in rigid body dynamics.