Find the principal moments of inertia of a flat rectangular plate of mass \(30 \mathrm{~g}\) and dimensions \(80 \mathrm{~mm} \times 60 \mathrm{~mm}\). Given that the plate is rotating about a diagonal with angular velocity \(15 \mathrm{rad} \mathrm{s}^{-1}\), find the components of the angular momentum parallel to the edges. Given that the axis is of total length \(120 \mathrm{~mm}\), and is held vertical by bearings at its ends, find the horizontal component of the force on each bearing.

Short Answer

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To solve this problem, we need to follow these steps: 1. Calculate the area moment of inertia about the x- and y-axis using the given mass and dimensions of the plate. 2. Find the principal moments of inertia using the formula \(I_p = (\sqrt{I_x^2 + I_y^2})\). 3. Determine the angle \(\theta\) between the diagonal axis and the x-axis, and find the components of angular velocity, \(\omega_x\) and \(\omega_y\). 4. Calculate the components of angular momentum parallel to the edges, \(L_x\) and \(L_y\), using the principal moments of inertia and the components of angular velocity. 5. Find the horizontal components of the force on each bearing, \(F_x\) and \(F_y\), using the calculated values of angular momentum and the given length of the axis. Keep in mind that these steps are a guide to the calculations, and it's essential to plug in the correct values and use the appropriate formulas to get an accurate answer.

Step by step solution

01

Calculating the Area Moment of Inertia

First, we need to find the area moment of inertia for the flat rectangular plate. For a rectangular plate, the moment of inertia about the x- and y-axis can be found using the formulas: \(I_x = (1/12)mb^2\) \(I_y = (1/12)ma^2\) Where \(m\) is the mass of the plate, \(a\) is the width, and \(b\) is the length. We are given the mass and dimensions of the plate, so we can plug those in and find the moments of inertia about the x- and y-axis.
02

Principal Moments of Inertia

Now, we can find the principal moments of inertia. The principal moments of inertia for a rectangle are given by the formula: \(I_p = (\sqrt{I_x^2 + I_y^2})\) We can plug in the values of \(I_x\) and \(I_y\) we found in Step 1 to find the principal moments of inertia, \(I_p\).
03

Angular Velocity Components

We are given the angular velocity of the plate, which is 15 rad/s. Since the plate is rotating about a diagonal, the components of angular velocity parallel to the edges can be found as follows: \(\omega_x = \omega \cos(\theta)\) \(\omega_y = \omega \sin(\theta)\) Where \(\theta\) is the angle between the diagonal axis and the x-axis. For a rectangle, this angle can be found using the tangent function: \(\tan(\theta) = \frac{b}{a}\) Calculate the angle \(\theta\), and then plug in the given values of \(\omega\) to find the components of angular velocity, \(\omega_x\) and \(\omega_y\).
04

Angular Momentum Components

Now, we can find the components of angular momentum parallel to the edges of the plate using the following formulas: \(L_x = I_p\omega_x\) \(L_y = I_p\omega_y\) Plug in the values of \(I_p\), \(\omega_x\), and \(\omega_y\) we found in the previous steps, to find the components of angular momentum, \(L_x\) and \(L_y\).
05

Horizontal Components of Force

Given that the axis is of total length 120 mm, and the force is distributed across two bearings on either end, we can find the horizontal component of the force on each bearing using the following formulas: \(F_x = \frac{L_x^2 + L_y^2}{2l}\) \(F_y = -\frac{L_x^2 + L_y^2}{2l}\) Where \(l\) is the length of the axis (120 mm). Plug in the values of \(L_x, L_y\), and \(l\) to find the components of the force on each bearing, \(F_x\) and \(F_y\).

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