/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 18 A person measures the time perio... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

A person measures the time period of a simple pendulum inside a stationary lift and finds it to be \(T\). If the lift starts accelerating upwards with an acceleration of \(\mathrm{g} / 3\), the time period of the pendulum will be (A) \(\sqrt{3} T\) (B) \(\frac{\sqrt{3}}{2} T\) (C) \(T / \sqrt{3}\) (D) \(T / 3\)

Short Answer

Expert verified
The new time period of the pendulum when the lift accelerates upwards with an acceleration of \(g/3\) is (B) \(\frac{\sqrt{3}}{2} T\).

Step by step solution

01

Recall the formula for the time period of a simple pendulum

The time period T of a simple pendulum is given by the formula: \(T = 2\pi \sqrt{\frac{l}{g}}\), where l is the length of the pendulum and g is the acceleration due to gravity.
02

Modify the formula considering the acceleration of the lift

When the lift accelerates upward with acceleration \(a = \frac{g}{3}\), the effective acceleration experienced by the pendulum is \(g' = g + a\). Therefore, the modified equation for the time period under acceleration is given by \(T' = 2\pi \sqrt{\frac{l}{g'}}\).
03

Substitute values for g and a

Substituting the given values for acceleration due to gravity (g) and the lift's upward acceleration (a) into the modified equation: \(T' = 2\pi \sqrt{\frac{l}{g + \frac{g}{3}}}\).
04

Simplify the equation

Simplify the equation: \(T' = 2\pi \sqrt{\frac{l}{\frac{4g}{3}}}\).
05

Compare the new time period with the original time period

To find the relation between T' and T, we'll compare the two equations: \(\frac{T'}{T} = \frac{2\pi \sqrt{\frac{l}{\frac{4g}{3}}}}{2\pi \sqrt{\frac{l}{g}}}\). Simplifying the equation, we get: \(\frac{T'}{T} = \sqrt{\frac{3}{4}}\).
06

Find the value of T'

Now, we can find the value of T' by multiplying both sides of the equation by T: \(T'= TT'\). Therefore, \(T' = \frac{\sqrt{3}}{2}T\). The correct answer is (B) \(\frac{\sqrt{3}}{2} T\).

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

For a certain stretched string, three consecutive resonance frequencies are observed as \(105,175,245 \mathrm{~Hz}\), respectively. Then select the correct alternatives (A) The string is fixed at both ends. (B) The string is fixed at one end only. (C) The fundamental frequency is \(35 \mathrm{~Hz}\). (D) The fundamental frequency is \(52.5 \mathrm{~Hz}\).

A particle starts SHM at time \(t=0 .\) Its amplitude is \(A\) and angular frequency is \(\omega .\) At time \(t=0\), its kinetic energy is \(\frac{E}{4}\), where \(E\) is total energy. Assuming potential energy to be zero at mean position, the displacement-time equation of the particle can be written as (A) \(x=A \cos \left(\omega t+\frac{\pi}{6}\right)\) (B) \(x=A \sin \left(\omega t+\frac{\pi}{3}\right)\) (C) \(x=A \sin \left(\omega t-\frac{2 \pi}{3}\right)\) (D) \(x=A \cos \left(\omega t-\frac{\pi}{6}\right)\)

Column-I (A) Beats (B) Standing waves (C) Interference (D) Echo Column-II 1\. Redistribution of energy 2\. Multiple reflection 3\. Varying amplitude 4\. Reflection from a rigid support

A particle of mass \(m\) is moving in a field where the potential energy is given by \(U(x)=U_{0}(1-\cos a x)\), where \(U_{0}\) and a are constants and \(x\) is the displacement from mean position. Then (for small oscillations) (A) The time period is \(T=2 \pi \sqrt{\frac{m}{a U_{0}}}\). (B) The speed of particle is maximum at \(x=0\). (C) The amplitude of oscillations is \(\underline{\pi}\). (D) The time period is \(T=2 \pi \sqrt{\frac{m}{a^{2} U_{0}}}\).

The general wave equation can be written as \(y=m(x-v t), x \in\left[v t, v t+\frac{a}{2}\right]$$y=-m[(x-v t)-a], x \in\left[v t+\frac{a}{2}, v t+a\right]\)

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.