/*! 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 73 A water droplet of radius 0.018\... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

A water droplet of radius 0.018\(\mathrm { mm }\) remains stationary in the air. If the downward-directed electric field of the Earth is \(150 \mathrm { N } / \mathrm { C } ,\) how many excess electron charges must the water droplet have?

Short Answer

Expert verified
Around 99,400 excess electrons are needed.

Step by step solution

01

Understand the Forces

The water droplet remains stationary, indicating that the net force acting on the droplet is zero. This means the gravitational force pulling it down is balanced by the electric force pushing it up.
02

Calculate the Gravitational Force

The gravitational force acting on the droplet can be calculated using the formula: \( F_g = mg \), where \( m \) is mass and \( g \) is the acceleration due to gravity (\(9.8 \, \mathrm{m/s^2}\)). First, find the mass \( m \) using \( m = \frac{4}{3} \pi r^3 \rho \), where \( r = 0.018 \, \mathrm { mm } = 0.018 \times 10^{-3} \, \mathrm{m} \) and \( \rho = 1000 \, \mathrm{kg/m^3} \) (density of water). \( m = \frac{4}{3} \pi (0.018 \times 10^{-3})^3 \times 1000 \approx 2.44 \times 10^{-13} \, \mathrm{kg} \). Thus, \( F_g \approx 2.44 \times 10^{-13} \, \times 9.8 \approx 2.39 \times 10^{-12} \, \mathrm{N}. \)
03

Calculate the Electric Force

The electric force \( F_e \) can be expressed as \( F_e = qE \), where \( q \) represents the charge and \( E = 150 \, \mathrm{N/C} \) is the electric field. Since \( F_e = F_g \), set the gravitational force equal to the electric force to find \( q \): \( q \approx \frac{2.39 \times 10^{-12}}{150} \approx 1.59 \times 10^{-14} \, \mathrm{C}. \)
04

Determine the Number of Excess Electrons

The charge \( q \) is due to excess electrons. The charge of one electron \( e \) is approximately \(-1.6 \times 10^{-19} \, \mathrm{C} \). The number of excess electrons \( n \) can be calculated using \( q = ne \). Thus, \( n \approx \frac{1.59 \times 10^{-14}}{1.6 \times 10^{-19}} \approx 9.94 \times 10^4 \).

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.

Gravitational Force
Imagine a water droplet suspended in the air. It's not falling or rising, just staying put. This is because the force pulling it down—the gravitational force—is perfectly balanced by another force pushing it up. Here, we dive into this invisible pull of gravity that keeps us grounded.

The gravitational force acting on an object is given by the formula:
  • \( F_g = mg \)
where:
  • \( F_g \) is the gravitational force,
  • \( m \) is the mass of the object, and
  • \( g \) is the acceleration due to gravity (approximately \(9.8 \, \mathrm{m/s^2}\) on Earth).
For our tiny water droplet, we must first find its mass. Using its radius and the density of water, we calculate the mass through the formula:
  • \( m = \frac{4}{3} \pi r^3 \rho \),
where:
  • \( r \) is the radius (converted from millimeters to meters), and
  • \( \rho \) is the density of water (\(1000\, \mathrm{kg/m^3}\)).
By inserting the numbers, we determine the gravitational force. This emphasizes how gravity affects objects no matter their size or weight, though its effects become more noticeable as mass increases.
Electric Force
Next, we have the electric force. This force is responsible for pushing our water droplet up in this scenario. Electric fields are everywhere, created by different charges. The Earth itself has a downward-directed electric field that affects various objects, including our droplet.

The force due to electricity is calculated through:
  • \( F_e = qE \)
where:
  • \( F_e \) is the electric force,
  • \( q \) is the charge on the object, and
  • \( E \) is the strength of the electric field (given here as \(150 \, \mathrm{N/C}\)).
In this balanced state for the droplet, the gravitational force and the electric force are equal, allowing us to solve for the charge \( q \) required to keep the droplet stationary. Understanding this interplay between electric and gravitational forces is crucial, as it showcases how electric fields can influence objects just as gravitation does, sometimes even counteracting it entirely.
Charge of an Electron
The world of electricity revolves around electrons, the tiny carriers of electric charge. Each electron holds a specific charge, which is approximately \(-1.6 \times 10^{-19} \, \mathrm{C}\). This negative charge is fundamental to understanding electric interactions.

When a water droplet like ours seems to levitate, it's due to excess electrons present in it, creating a net charge. We determine how many of these electrons are needed by using the formula:
  • \( q = ne \),
where:
  • \( n \) is the number of excess electrons, and
  • \( e \) is the charge of one electron.
By knowing the total charge \( q \) needed to balance the gravitational pull, we can divide it by the charge of a single electron to find \( n \). These calculations highlight the integral role electrons play in the behavior of charged objects, showcasing how such tiny particles can significantly influence the macroscopic world around us.

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

(III) A thin glass rod is a semicircle of radius \(R\), Fig. \(21-66\). A charge is nonuniformly distributed along the rod with a linear charge density given by \(\lambda=\lambda_{0} \sin \theta,\) where \(\lambda_{0}\) is a positive constant. Point \(\mathbf{P}\) is at the center of the semicircle. (a) Find the electric field \(\overrightarrow{\mathbf{E}}\) (magnitude and direction) at point P. [Hint: Remember \(\sin (-\theta)=-\sin \theta,\) so the two halves of the rod are oppositely charged.] (b) Determine the acceleration \(\quad\) (magnitude \(\quad\) and direction) of an electron placed at point \(\mathrm{P},\) assuming \(\quad R=1.0 \mathrm{~cm}\) and \(\lambda_{0}=1.0 \mu \mathrm{C} / \mathrm{m}\)

(II) Calculate the electric field at the center of a square \(52.5 \mathrm{~cm}\) on a side if one corner is occupied by a \(-38.6 \mu \mathrm{C}\) charge and the other three are occupied by \(-27.0 \mu \mathrm{C}\) charges.

(a) The electric field near the Earth's surface has magnitude of about \(150 \mathrm{~N} / \mathrm{C} .\) What is the acceleration experienced by an electron near the surface of the Earth? (b) What about a proton? (c) Calculate the ratio of each acceleration to \(g=9.8 \mathrm{~m} / \mathrm{s}^{2}\)

(II) Estimate the electric field at a point 2.40\(\mathrm { cm }\) perpendicular to the midpoint of a uniformly charged 2.00 -m-long thin wire carrying a total charge of 4.75\(\mu \mathrm { C }\) .

(II) What is the electric field strength at a point in space where a proton experiences an acceleration of 1.8 million "g's"?

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.