/*! 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 53 One kilogram of glass \(\left(\r... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

One kilogram of glass \(\left(\rho=2.60 \times 10^{3} \mathrm{kg} / \mathrm{m}^{3}\right)\) is shaped into a hollow spherical shell that just barely floats in water. What are the inner and outer radii of the shell? Do not assume that the shell is thin.

Short Answer

Expert verified
Outer radius \(R \approx 0.0620\) m, inner radius \(r \approx 0.0503\) m.

Step by step solution

01

Calculate the volume of the glass

First, determine the volume of glass forming the shell using the given density. The density \(\rho\) formula is \(\rho = \frac{m}{V}\), where \(m\) is the mass and \(V\) is the volume. Given \(m = 1 \text{ kg}\) and \(\rho = 2.60 \times 10^{3} \text{ kg/m}^3\), solve for \(V\): \[V = \frac{m}{\rho} = \frac{1}{2.60 \times 10^{3}} \approx 3.85 \times 10^{-4} \text{ m}^3.\]
02

Understand the condition for floating

For the sphere to float, the weight of the displaced water must equal the weight of the sphere. This means \(\rho_{w} V_{out} g = m g\), where \(\rho_{w}\) is the density of water (approximately \(1000 \text{ kg/m}^3\)), and \(V_{out}\) is the volume displaced by the entire sphere.
03

Calculate the outer volume

From the floating condition, \(V_{out} = \frac{m}{\rho_{w}} = \frac{1}{1000} = 10^{-3} \text{ m}^3\). This is the volume of water displaced, equivalent to the volume of the sphere with the outer radius.
04

Formulate the radii equations

The volume of the hollow spherical shell is given by the difference between the volumes of two spheres: \(V_{out} - V_{in} = V\), where \(V_{out}\) corresponds to the sphere with radius \(R\), and \(V_{in}\) corresponds to the inside volume with radius \(r\). Thus, \[ \frac{4}{3}\pi R^3 - \frac{4}{3}\pi r^3 = 3.85 \times 10^{-4}. \]
05

Solve the system of equations

We now have two equations: 1. \( \frac{4}{3} \pi R^3 = 10^{-3} \)2. \( \frac{4}{3} \pi (R^3 - r^3) = 3.85 \times 10^{-4} \)Solve the first to find \( R^3 = \frac{3 \times 10^{-3}}{4\pi} \) and substitute in the second equation to find \( r^3 = R^3 - \left(\frac{3 \times 3.85 \times 10^{-4}}{4\pi}\right) \).
06

Calculate the radii

Substituting the values from the previous equations, calculate:\( R^3 = (\frac{3 \times 10^{-3}}{4\pi})\) and\( r^3 = R^3 - (\frac{3 \times 3.85 \times 10^{-4}}{4\pi})\). Use a calculator to determine \(R\) and \(r\). You'll find that \(R \approx 0.0620 \text{ m}\) and \(r \approx 0.0503 \text{ m}\).

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.

Density
Density is a fundamental concept used to measure how much mass is contained in a given volume. It is defined as the mass per unit volume and is mathematically represented as \( \rho = \frac{m}{V} \), where \( \rho \) is the density, \( m \) is the mass, and \( V \) is the volume. In the context of the hollow spherical shell problem, the density of glass is given as \( 2.60 \times 10^{3} \, \text{kg/m}^3 \). Since the mass of the glass is known to be 1 kilogram, you can calculate the volume of the glass by rearranging the formula to solve for \( V \): \( V = \frac{m}{\rho} \).
This calculation is crucial for determining the volume that the glass occupies when forming the shell.
The understanding of this concept aids in solving problems where you need to find one of the three properties if the other two are known.
Volume Calculation
Volume calculation is essential when determining the dimensions required for a specific shape or structure.
For the hollow spherical shell, it is crucial to calculate both the outer and inner volumes to find the respective radii. The outer volume \( V_{out} \) corresponds to the volume of water displaced, which is based on the condition for floating. In this problem, it is found using the formula: \( V_{out} = \frac{1}{\rho_w} \), where \( \rho_w \) is the density of water. This gives a volume of \( 10^{-3} \, \text{m}^3 \).
The inner volume \( V_{in} \), on the other hand, is calculated as the difference between the outer volume and the volume of glass (hollow portion): \( V = \frac{4}{3}\pi R^3 - \frac{4}{3}\pi r^3 \); where \( R \) and \( r \) are the outer and inner radii, respectively.Understanding how to calculate these volumes is essential for assessing the spatial requirements of the shell and is foundational in fluid mechanics problems involving buoyancy.
Floating Condition
The principle of buoyancy explains how and why objects float. Derived from Archimedes' Principle, it states that for an object to float, the weight of the fluid displaced by the object must be equal to the weight of the object itself. This is the condition required for the hollow spherical shell to float in water.
In mathematical terms, the condition can be expressed as \( \rho_w \times V_{out} \times g = m \times g \). Here, \( \rho_w \) is the density of water, \( V_{out} \) is the volume of the sphere's outer surface (the total volume displaced), and \( \text{g} \) is the acceleration due to gravity.
This results in finding the volume of water displaced as equal to the mass divided by the density of water: \( V_{out} = \frac{m}{\rho_w} = 10^{-3} \, \text{m}^3 \). Understanding this floating condition helps in visualizing the balance of forces that allows the spherical shell to float and further guides in solving equations involving its dimensions.
Hollow Spherical Shell
A hollow spherical shell consists of two concentric spheres: an outer sphere and an inner sphere, with a cavity in between. The difference in volumes between these spheres defines the material volume forming the shell. In the exercise provided, this structure is vital for understanding how the shell floats and holds its shape.A critical aspect of dealing with hollow spherical shells is the radii differencing formula: \( V_{out} - V_{in} = V \) where \( V \) is the volume of the glass forming the shell, calculated from density and mass. The physical condition \( \frac{4}{3} \pi R^3 = 10^{-3} \), derived from floating, sets the equation for the outer radius.The process involves using traditional geometric volume formulas for spheres: \( \frac{4}{3} \pi R^3 \) and \( \frac{4}{3} \pi r^3 \). Solving these simultaneously allows for finding the two radii, helping visualize how the shell forms a balance between material used and space displaced.This understanding of a hollow spherical structure aids in problems across physics and engineering, providing a clear illustration of space and matter interaction in three-dimensional geometric shapes.

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

Multiple-Concept Example 8 presents an approach to problems of this kind. The hydraulic oil in a car lift has a density of \(8.30 \times 10^{2} \mathrm{kg} / \mathrm{m}^{3}\). The weight of the input piston is negligible. The radii of the input piston and output plunger are \(7.70 \times 10^{-3} \mathrm{m}\) and \(0.125 \mathrm{m},\) respectively. What input force \(F\) is needed to support the \(24500-\mathrm{N}\) combined weight of a car and the output plunger, when (a) the bottom surfaces of the piston and plunger are at the same level, and (b) the bottom surface of the output plunger is \(1.30 \mathrm{m}\) above that of the input piston?

A small crack occurs at the base of a 15.0 -m-high dam. The effective crack area through which water leaves is \(1.30 \times 10^{-3} \mathrm{m}^{2}\) (a) Ignoring viscous losses, what is the speed of water flowing through the crack? (b) How many cubic meters of water per second leave the dam?

A solid concrete block weighs 169 N and is resting on the ground. Its dimensions are \(0.400 \mathrm{m} \times 0.200 \mathrm{m} \times 0.100 \mathrm{m} .\) A number of identical blocks are stacked on top of this one. What is the smallest number of whole blocks (including the one on the ground) that can be stacked so that their weight creates a pressure of at least two atmospheres on the ground beneath the first block?

A log splitter uses a pump with hydraulic oil to push a piston, which is attached to a chisel. The pump can generate a pressure of \(2.0 \times 10^{7} \mathrm{Pa}\) in the hydraulic oil, and the piston has a radius of \(0.050 \mathrm{m}\). In a stroke lasting \(25 \mathrm{s},\) the piston moves \(0.60 \mathrm{m} .\) What is the power needed to operate the log splitter's pump?

One way to administer an inoculation is with a "gun" that shoots the vaccine through a narrow opening. No needle is necessary, for the vaccine emerges with sufficient speed to pass directly into the tissue beneath the skin. The speed is high, because the vaccine \(\left(\rho=1100 \mathrm{kg} / \mathrm{m}^{3}\right)\) is held in a reservoir where a high pressure pushes it out. The pressure on the surface of the vaccine in one gun is \(4.1 \times 10^{6}\) Pa above the atmospheric pressure outside the narrow opening. The dosage is small enough that the vaccine's surface in the reservoir is nearly stationary during an inoculation. The vertical height between the vaccine's surface in the reservoir and the opening can be ignored. Find the speed at which the vaccine emerges.

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.