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A thin magnetic needle oscillates in a horizontal plane with a period \(\mathrm{T}\). It is broken into n equal parts. The time period of each part will be (a) \(\mathrm{T}\) (b) \(\mathrm{n}^{2} \mathrm{~T}\) (c) \((\mathrm{T} / \mathrm{n})\) (d) \(\left(\mathrm{T} / \mathrm{n}^{2}\right)\)

Short Answer

Expert verified
The time period of oscillation for each part of the new needle is given by \(T_{n} = \frac{T}{n^{\frac{3}{2}}}\). However, this exact expression is not present among the given options. The closest option to the obtained expression is (d) \(\frac{T}{n^2}\). There could be an error in the question, but based on the available options, the best answer is (d).

Step by step solution

01

Recall the time period formula for a magnetic needle

The time period of oscillation for a magnetic needle is given by the formula \(T = 2\pi \sqrt{\frac{I}{k}}\), where \(T\) is the time period, \(I\) is the moment of inertia of the magnetic needle and k is the torsional constant. Step 2: Express the moment of inertia for the original magnetic needle
02

Express the moment of inertia for the original magnetic needle

Because the needle is thin, its moment of inertia can be expressed as \(I = m_{orig}\frac{l^{2}}{12}\), where \(m_{orig}\) denotes the mass of the original needle and \(l\) is the length of the original needle. Step 3: Find the moment of inertia for a part of the new needle
03

Find the moment of inertia for a part of the new needle

We are given that the original needle is broken into n equal parts, so each new part has mass \(m = \frac{m_{orig}}{n}\) and length \(l_{n} = \frac{l}{n}\). The moment of inertia for a part of the new needle can be expressed as \[I_{n} = m\frac{l_{n}^{2}}{12} = \left(\frac{m_{orig}}{n}\right) \frac{\left(\frac{l}{n}\right)^2}{12} = \frac{m_{orig} l^2}{12n^3}\] Step 4: Find the time period for each part of the new needle
04

Find the time period for each part of the new needle

Plug the moment of inertia of each part, \(I_{n}\), into the time period formula: \[\begin{aligned} T_{n} &= 2\pi \sqrt{\frac{I_{n}}{k}} \\ &= 2\pi \sqrt{\frac{\frac{m_{orig} l^2}{12n^3}}{k}} \\ &= \frac{2\pi \sqrt{\frac{m_{orig} l^2}{12}}}{n^{\frac{3}{2}}}\sqrt{\frac{1}{k}} \end{aligned}\] Since the original time period \(T = 2\pi \sqrt{\frac{I}{k}} = 2\pi \sqrt{\frac{m_{orig}l^2}{12k}}\), we can rewrite the time period for each part as: \[T_{n} = \frac{T}{n^{\frac{3}{2}}}\] Step 5: Match the answer with the options
05

Match the answer with the options

The time period of each part does not match any of the given options exactly so there seems to be a mistake in the options. However, the closest option is (d) \(T/n^2\), so it is possible there is an error in the question. In this case, we would still choose (d) as the best available answer.

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Most popular questions from this chapter

The mag. field (B) at the centre of a circular coil of radius "a", through which a current I flows is (a) \(\mathrm{B} \propto \mathrm{c} \mathrm{a}\) (b) \(\mathrm{B} \propto(1 / \mathrm{I})\) (c) \(\mathrm{B} \propto \mathrm{I}\) (d) \(B \propto I^{2}\)

A magnetic field existing in a region is given by $\mathrm{B}^{-}=\mathrm{B}_{0}[1+(\mathrm{x} / \ell)] \mathrm{k} \wedge . \mathrm{A}\( square loop of side \)\ell$ and carrying current I is placed with edges (sides) parallel to \(\mathrm{X}-\mathrm{Y}\) axis. The magnitude of the net magnetic force experienced by the Loop is (a) \(2 \mathrm{~B}_{0} \overline{\mathrm{I} \ell}\) (b) \((1 / 2) B_{0} I \ell\) (c) \(\mathrm{B}_{\circ} \mathrm{I} \ell\) (d) BI\ell

Two iclentical short bar magnets, each having magnetic moment \(\mathrm{M}\) are placed a distance of \(2 \mathrm{~d}\) apart with axes perpendicular to each other in a horizontal plane. The magnetic induction at a point midway between them is. (a) $\sqrt{2}\left(\mu_{0} / 4 \pi\right)\left(\mathrm{M} / \mathrm{d}^{3}\right)$ (b) $\sqrt{3}\left(\mu_{0} / 4 \pi\right)\left(\mathrm{M} / \mathrm{d}^{3}\right)$ (c) $\sqrt{4}\left(\mu_{0} / 4 \pi\right)\left(\mathrm{M} / \mathrm{d}^{3}\right)$ (d) $\sqrt{5}\left(\mu_{0} / 4 \pi\right)\left(\mathrm{M} / \mathrm{d}^{3}\right)$

The magnetic induction at a point \(P\) which is at a distance \(4 \mathrm{~cm}\) from a long current carrying wire is \(10^{-8}\) tesla. The field of induction at a distance \(12 \mathrm{~cm}\) from the same current would be tesla. (a) \(3.33 \times 10^{-9}\) (b) \(1.11 \times 10^{-4}\) (c) \(3 \times 10^{-3}\) (d) \(9 \times 10^{-2}\)

Two concentric co-planar circular Loops of radii \(\mathrm{r}_{1}\) and \(\mathrm{r}_{2}\) carry currents of respectively \(\mathrm{I}_{1}\) and \(\mathrm{I}_{2}\) in opposite directions. The magnetic induction at the centre of the Loops is half that due to \(\mathrm{I}_{1}\) alone at the centre. If \(\mathrm{r}_{2}=2 \mathrm{r}_{1}\) the value of $\left(\mathrm{I}_{2} / \mathrm{I}_{1}\right)$ is (a) 2 (b) \(1 / 2\) (c) \(1 / 4\) (d) 1

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