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Two point masses of \(0.3 \mathrm{~kg}\) and \(0.7 \mathrm{~kg}\) are fixed at the ends of a rod of length \(1.4 \mathrm{~m}\) and of negligible mass. The rod is set rotating about an axis perpendicular to its length with a uniform angular speed. The point on the rod through which the axis should pass in order that the work required for rotation of the rod is minimum, is located at a distance of ..... \(\\{\mathrm{A}\\} 0.4 \mathrm{~m}\) from mass of \(0.3 \mathrm{~kg}\) \\{B \(0.98 \mathrm{~m}\) from mass of \(0.3 \mathrm{~kg}\) \\{C\\} \(0.7 \mathrm{~m}\) from mass of \(0.7 \mathrm{~kg}\) \\{D \(\\} 0.98 \mathrm{~m}\) from mass of \(0.7 \mathrm{~kg}\)

Short Answer

Expert verified
The correct answer is \(\\{\mathrm{B}\\} 0.98 \mathrm{~m}\) from mass of \(0.3 \mathrm{~kg}\).

Step by step solution

01

Determine the moment of inertia

Moment of inertia, denoted by I, is the property of an object to resist change in its angular motion. For a point mass rotating about an axis parallel to its length, the moment of inertia is given by the mass times the square of the distance from the axis to the point mass, i.e. \(I = md^2\). In our case, we have two point masses, so the net moment of inertia would be the sum of the individual moments of inertia. For mass \(m_1 = 0.3 \mathrm{~kg}\), let the distance from the axis to the mass be d. The moment of inertia for this mass is \(I_1 = m_1 d^2\). For mass \(m_2 = 0.7 \mathrm{~kg}\), since the total length of the rod is \(1.4 \mathrm{~m}\), the distance from the axis to this mass would be \(1.4 \mathrm{~-} d\). The moment of inertia for this mass is \(I_2 = m_2 (1.4 - d)^2\). The net moment of inertia is given by \(I = I_1 + I_2\).
02

Differentiate the moment of inertia with respect to distance

Next, we need to minimize the moment of inertia I with respect to the distance d. To do this, we'll differentiate I with respect to d and set the derivative equal to 0. Therefore, \(\frac{dI}{dd} = \frac{d}{dd}(0.3d^2 + 0.7(1.4-d)^2) = 0\).
03

Solve for distance

Now, we need to solve the equation obtained in step 2 for the distance d. \(\frac{d}{dd}(0.3d^2 + 0.7(1.4-d)^2) = 0.6d - 1.4(0.7) + 1.4(0.7)d = 0\) Simplifying and solving for d, we get: \(d(d(0.6 + 0.7\cdot1.4) = 1.4(0.7)\) \(d = \frac{1.4(0.7)}{0.6 + 0.7(1.4)}\) \(d = 0.98 \mathrm{~m}\) According to the answer, the distance of 0.98 m is from mass \(0.3 \mathrm{~kg}\), which corresponds to option B. Thus, the correct answer is: \(\\{\mathrm{B}\\} 0.98 \mathrm{~m}\) from mass of \(0.3 \mathrm{~kg}\)

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Most popular questions from this chapter

Initial angular velocity of a circular disc of mass \(\mathrm{M}\) is \(\omega_{1}\) Then two spheres of mass \(\mathrm{m}\) are attached gently two diametrically opposite points on the edge of the disc what is the final angular velocity of the disc? \(\\{\mathrm{A}\\}[(\mathrm{M}+\mathrm{m}) / \mathrm{M}] \omega_{1}\) \(\\{\mathrm{B}\\}[(\mathrm{M}+4 \mathrm{~m}) / \mathrm{M}] \omega_{1}\) \(\\{\mathrm{C}\\}[\mathrm{M} /(\mathrm{M}+4 \mathrm{~m})] \omega_{1}\) \\{D\\} \([\mathrm{M} /(\mathrm{M}+2 \mathrm{~m})] \omega_{1}\)

Identify the correct statement for the rotational motion of a rigid body \(\\{A\\}\) Individual particles of the body do not undergo accelerated motion \\{B \\} The centre of mass of the body remains unchanged. \\{C\\} The centre of mass of the body moves uniformly in a circular path \\{D\\} Individual particle and centre of mass of the body undergo an accelerated motion.

The M.I of a disc of mass \(\mathrm{M}\) and radius \(\mathrm{R}\) about an axis passing through the centre \(\mathrm{O}\) and perpendicular to the plane of disc is \(\left(\mathrm{MR}^{2} / 2\right)\). If one quarter of the disc is removed the new moment of inertia of disc will be..... \(\\{\mathrm{A}\\}\left(\mathrm{MR}^{2} / 3\right)\) \(\\{B\\}\left(M R^{2} / 4\right)\) \(\\{\mathrm{C}\\}(3 / 8) \mathrm{MR}^{2}\) \(\\{\mathrm{D}\\}(3 / 2) \mathrm{MR}^{2}\)

The centre of mass of a systems of two particles is (A) on the line joining them and midway between them (B) on the line joining them at a point whose distance from each particle is proportional to the square of the mass of that particle. (C) on the line joining them at a point whose distance from each particle inversely proportional to the mass of that particle. (D) On the line joining them at a point whose distance from each particle is proportional to the mass of that particle.

The moment of inertia of a hollow sphere of mass \(\mathrm{M}\) and inner and outer radii \(\mathrm{R}\) and \(2 \mathrm{R}\) about the axis passing through its centre and perpendicular to its plane is \(\\{\mathrm{A}\\}(3 / 2) \mathrm{MR}^{2}\) \\{B \(\\}(13 / 32) \mathrm{MR}^{2}\) \(\\{\mathrm{C}\\}(31 / 35) \mathrm{MR}^{2}\) \(\\{\mathrm{D}\\}(62 / 35) \mathrm{MR}^{2}\)

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