/*! 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 42 A particle moves in a circle of ... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

A particle moves in a circle of radius \(R=\operatorname{lm}\) such that its spced varics with time as \(v=0.5 e^{t} \mathrm{~m} / \mathrm{s}\). Find the initial acccleration of the particle.

Short Answer

Expert verified
The initial acceleration of the particle is approximately 0.559 m/s².

Step by step solution

01

Define the Given Variables

We are given that the radius of the circle, \(R = 1 \text{ m}\), and the particle's speed as a function of time is given by \(v = 0.5e^{t} \text{ m/s}\).
02

Understand the Acceleration Components

The acceleration of a particle moving in a circle has two components: tangential acceleration \(a_t\) and centripetal (radial) acceleration \(a_c\). The total acceleration \(a\) can be found by combining these components: \(a = \sqrt{a_t^2 + a_c^2}\).
03

Find the Tangential Acceleration

Tangential acceleration \(a_t\) is the rate of change of speed. It can be found by taking the derivative of the speed function with respect to time. Calculate \(a_t = \frac{dv}{dt} = \frac{d}{dt}(0.5e^t) = 0.5e^t\). At \(t=0\), \(a_t = 0.5 \text{ m/s}^2\).
04

Find the Centripetal Acceleration

Centripetal acceleration \(a_c\) is given by \(a_c = \frac{v^2}{R}\). At \(t=0\), \(v = 0.5 \text{ m/s}\), so \(a_c = \frac{(0.5)^2}{1} = 0.25 \text{ m/s}^2\).
05

Calculate the Initial Total Acceleration

Using the tangential and centripetal components, the total acceleration \(a\) can be computed as \(a = \sqrt{a_t^2 + a_c^2} = \sqrt{(0.5)^2 + (0.25)^2} = \sqrt{0.25 + 0.0625} = \sqrt{0.3125}\). Calculate \(\sqrt{0.3125} \approx 0.559 \text{ m/s}^2\).

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!

Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Tangential Acceleration
In circular motion, tangential acceleration refers to the change in speed along the circular path. Imagine a particle racing around a track, where it's either speeding up or slowing down at different moments. This change in speed is what we call tangential acceleration.
  • Tangential acceleration involves changes in the speed of the particle along the tangent to the circle.
  • Mathematically, it is the derivative of the speed function with respect to time.
To find this, you can start by taking the function for speed. In our exercise, the speed is given as a function of time: \[ v = 0.5e^{t} \] By differentiating this function with respect to time, you obtain the particle's rate of change of speed at any moment. \[ a_t = \frac{dv}{dt} = 0.5e^{t} \] When you substitute \( t=0 \), you'll get the initial tangential acceleration, which here is: \[ a_t = 0.5 \text{ m/s}^2 \] This means that right at the start, the particle is speeding up along the circle's path at \( 0.5 \text{ m/s}^2 \).
Centripetal Acceleration
Centripetal acceleration is another critical aspect of circular motion. While tangential acceleration deals with changes in speed, centripetal acceleration is all about direction. It keeps the particle moving along its circular path by constantly changing the direction of its velocity.
  • Always points towards the center of the circle.
  • Depends on both the speed of the particle and the radius of the circle.
In this exercise, centripetal acceleration is calculated using the formula: \[ a_c = \frac{v^2}{R} \] When you plug in the values given at \( t=0 \), with \( v = 0.5 \text{ m/s} \) and \( R = 1 \text{ m} \), you get: \[ a_c = \frac{(0.5)^2}{1} = 0.25 \text{ m/s}^2 \] Thus, the particle experiences a centripetal acceleration of \( 0.25 \text{ m/s}^2 \) towards the center of the circle, ensuring it stays on its circular path.
Initial Acceleration Calculation
Now, let's combine our understanding of both tangential and centripetal acceleration to find the total initial acceleration of the particle. In circular motion, these two components are perpendicular to each other, and they combine to give the total acceleration.
  • The total acceleration is obtained by the Pythagorean sum of the tangential and centripetal components.
For our particle at \( t=0 \), using previously calculated values of \( a_t = 0.5 \text{ m/s}^2 \) and \( a_c = 0.25 \text{ m/s}^2 \):\[ a = \sqrt{a_t^2 + a_c^2} \] Place these values into the formula:\[ a = \sqrt{(0.5)^2 + (0.25)^2} = \sqrt{0.25 + 0.0625} = \sqrt{0.3125} \] So, the initial total acceleration comes out to be approximately \( 0.559 \text{ m/s}^2 \). This result tells us how both the change in speed and the direction contribute to the particle's acceleration at the start of its journey around the circle.

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

What is the average velocity of a particle projected from the ground with speed \(u\) at an angle \(\alpha\) with the horizontal over a time interval from beginning till it strikes the ground again?

In uniform circular motion a body moves with constant speed \(v\) on a circular path of constant radius \(r\). In this motion Column-I (a) The acceleration of body is (b) The kinetic energy (c) The angular displacement of body at any instant is directed along (d) The velocity of body is always directed along Column-II (p) tangent to path at evety point (q) alng axis of rotation (r) constant in magnitude but changing in direction (s) constant always

A body moving with a constant speod describes a circular path whose radius vector is given by \(\vec{r}-15(\cos p t \hat{i}+\sin p t \hat{j}) \mathrm{m}\) where \(p\) is in \(\mathrm{rad} / \mathrm{s}\), and \(t\) is in second. What is its centripetal acecleration at \(\ell=3 \mathrm{~s}\) ? (a) \(\left(45 p^{2}\right) \mathrm{m} / \mathrm{s}^{2}\) (b) \(\left(5 p^{2}\right) \mathrm{m} / \mathrm{s}^{3}\) (c) \((15 p) \mathrm{m} / \mathrm{s}^{2}\) (d) \(\left(15 p^{2}\right) \mathrm{m} / \mathrm{s}^{2}\)

Three particles are projected simultaneously and in the same vertical plane with different velocities and at different angles. Show that the area of the triangle formed by the particles at time \(t\) is proportional to \(t^{2}\).

Two towns \(A\) and \(B\) are connccled by a regular bus service with a bus leaving in cither dircetion cvery \(T\) minutes. A man cycling with a speed of \(20 \mathrm{~km} / \mathrm{h}\) in the dircction \(A\) to \(B\) notices that a bus goes past him cvery \(18 \mathrm{~min}\). in the dircction of his motion and cvery \(6 \mathrm{~min}\). in the opposite dircetion. What is the period \(T\) o \([\) the bus serviec and with what spod (assumed constant) do the buses ply on the road?

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.