/*! 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 25 Find the density \(\rho\) of a f... [FREE SOLUTION] | 91Ó°ÊÓ

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Find the density \(\rho\) of a fluid at a depth \(h\) in terms of its density \(\rho_{0}\) at the surface. If a mass \(m\) of fluid has volume \(V_{0}\) at the surface, then it will have volume \(V_{0}-\Delta V\) at a depth \(h\). The density at depth \(h\) is then which gives $$ \begin{array}{c} \rho=\frac{m}{V_{0}-\Delta V} \quad \text { while } \quad \rho_{0}=\frac{m}{V_{0}} \\ \frac{\rho}{\rho_{0}}=\frac{V_{0}}{V_{0}-\Delta V}=\frac{1}{1-\left(\Delta V / V_{0}\right)} \end{array} $$ However, from Chapter 12, the bulk modulus is \(B=P /\left(\Delta V / V_{0}\right)\) and so \(\Delta V / V_{0}=P / B\). Making this substitution, we obtain $$ \frac{\rho}{\rho_{0}}=\frac{1}{1-P / B} $$ If we assume that \(\rho\) is close to \(\rho 0\), then the pressure at depth \(h\) is approximately \(\rho_{0} g h\), and so $$ \frac{\rho}{\rho_{0}}=\frac{1}{1-\left(\rho_{0} g h / B\right)} $$

Short Answer

Expert verified
The fluid density at depth is \( \rho = \frac{\rho_0}{1 - (\rho_0 gh / B)} \).

Step by step solution

01

Understand the Problem

We're tasked to find the density \( \rho \) of a fluid at a depth \( h \) given its surface density \( \rho_0 \). The relationship involves changes in fluid volume at depth due to pressure differences.
02

Define Initial Relationships

At the surface, the fluid density is given by \( \rho_0 = \frac{m}{V_{0}} \), where \( m \) is mass and \( V_{0} \) is the volume. At a depth \( h \), the density is \( \rho = \frac{m}{V_{0} - \Delta V} \), indicating that volume changes affect density.
03

Express Density Ratio

The density ratio at depth \( h \) is \( \frac{\rho}{\rho_{0}} = \frac{V_{0}}{V_{0} - \Delta V} \). Using the bulk modulus relationship, we know that \( \Delta V / V_{0} = P / B \), which allows rewriting the density ratio as \( \frac{\rho}{\rho_{0}} = \frac{1}{1 - P/B} \).
04

Substitute Pressure and Simplify

We substitute \( P \approx \rho_{0}gh \) where \( g \) is the acceleration due to gravity and \( h \) is the depth, leading to the equation \( \frac{\rho}{\rho_{0}} = \frac{1}{1 - (\rho_{0} gh / B)} \). This expression gives the fluid density at depth in terms of surface density and depth.

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Key Concepts

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

Understanding Bulk Modulus
The bulk modulus is a measure of a material's resistance to uniform compression. It is a critical concept when studying fluids because it describes how a fluid's volume changes under pressure. Mathematically, the bulk modulus, denoted by \( B \), is defined as the ratio of pressure increase \( P \) to the relative decrease in volume, expressed as:\[ B = \frac{P}{\Delta V/V_0} \]where \( \Delta V/V_0 \) represents the fractional change in volume relative to the original volume \( V_0 \).
This property helps us quantify how compressible a fluid is. A large bulk modulus indicates a fluid is less compressible, meaning that even when high pressure is applied, the fluid's volume doesn't change much. This principle is essential while considering how pressure affects fluid density at different depths.
Pressure Depth Relationship in Fluids
In fluids, the deeper you go, the greater the pressure. This is known as the pressure depth relationship. This fundamental concept states that pressure at a certain depth \( h \) is given by:\[ P = \rho_0 g h \]Here, \( \rho_0 \) is the fluid's density at the surface, \( g \) is the acceleration due to gravity, and \( h \) is the depth. This equation shows that pressure increases linearly with depth.
This increase in pressure affects the fluid's volume and consequently its density. Understanding this relationship helps us predict how a fluid’s properties might change in environments like deep oceans or high-pressure containers.
Density Ratio and Its Importance
The density ratio in this context compares how the fluid density at depth \( \rho \) compares to that at the surface \( \rho_0 \). This ratio is crucial for understanding changes in fluid properties under pressure:\[ \frac{\rho}{\rho_0} = \frac{1}{1 - (\rho_0 gh / B)} \]This equation results from considering how pressure affects volume and thus density, and it incorporates the bulk modulus \( B \).
By calculating this ratio, one can determine how much denser a fluid becomes when subjected to the increased pressure at greater depths. It's a practical formula found in many physics and engineering applications, such as hydraulic systems and fluid dynamics.
Volume Change Due to Pressure
When a fluid is subjected to pressure, its volume changes slightly, and this relationship is described using the concept of compressibility. The change in volume \( \Delta V \) at a given depth from the initial volume \( V_0 \) is given by:\[ \frac{\Delta V}{V_0} = \frac{P}{B} \]This expression comes from the bulk modulus, indicating how much the volume decreases relative to the pressure applied. The smaller the volume change, the higher the compressibility resistance the fluid possesses.
This is important in calculating how dense a fluid becomes when compressed. Knowing how pressure affects volume helps predict how fluid density changes in practical applications, such as predicting sea water density changes with depth.

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Most popular questions from this chapter

What must be the volume \(V\) of a \(5.0\) -kg balloon filled with helium \(\left(\rho_{\mathrm{He}}=0.178 \mathrm{~kg} / \mathrm{m}^{3}\right)\) if it is to lift a 30 -kg load? Use \(\rho_{\text {air }}=\) \(1.29 \mathrm{~kg} / \mathrm{m}^{3}\) The buoyant force, \(V \rho_{\text {airg }}\), must lift the weight of the balloon, its load, and the helium within it: $$ V \rho_{\text {air }} g=(35 \mathrm{~kg})(g)+V \rho_{\mathrm{He}} g $$ which gives $$ V=\frac{35 \mathrm{~kg}}{\rho_{\text {air }}-\rho_{\mathrm{He}}}=\frac{35 \mathrm{~kg}}{1.11 \mathrm{~kg} / \mathrm{m}^{3}}=32 \mathrm{~m}^{3} $$

How high would water rise in the essentially open pipes of a building if the water pressure gauge shows the pressure at the ground floor to be \(270 \mathrm{kPa}\) (about \(40 \mathrm{lb} / \mathrm{in}^{2}\).)? Water pressure gauges read the excess pressure just due to the water, that is, the difference between the absolute pressure in the water and the pressure of the atmosphere. The water pressure at the bottom of the highest column that can be supported is \(270 \mathrm{kPa}\). Therefore, \(P=\rho_{w} p h\) gives $$ h=\frac{P}{\rho_{w} g}=\frac{2.70 \times 10^{5} \mathrm{~N} / \mathrm{m}^{2}}{\left(1000 \mathrm{~kg} / \mathrm{m}^{3}\right)\left(9.81 \mathrm{~m} / \mathrm{s}^{2}\right)}=27.5 \mathrm{~m} $$

A glass of water has a \(10-\mathrm{cm}^{3}\) ice cube floating in it. The glass is filled to the brim with cold water. By the time the ice cube has completely melted, how much water will have flowed out of the glass? The sp gr of ice is \(0.92\).

A vertical test tube has \(2.0 \mathrm{~cm}\) of oil \(\left(\rho=0.80 \mathrm{~g} / \mathrm{cm}^{3}\right)\) floating on \(8.0 \mathrm{~cm}\) of water. What is the pressure at the bottom of the tube due to the liquid in it? $$ \begin{aligned} P &=\rho_{1} h h_{1}+\rho_{2} h_{2}=\left(800 \mathrm{~kg} / \mathrm{m}^{3}\right)\left(9.81 \mathrm{~m} / \mathrm{s}^{2} \times 0.020 \mathrm{~m}\right)+\left(1000 \mathrm{~kg} / \mathrm{m}^{3}\right)\left(9.81 \mathrm{~m} / \mathrm{s}^{2}\right)(0.080 \mathrm{~m}) \\ &=0.94 \mathrm{kPa} \end{aligned} $$

A spring whose composition is not completely known might be either bronze (sp gr \(8.8\) ) or brass (sp gr \(8.4\) ). It has a mass of \(1.26\) g when measured in air and \(1.11\) g in water. Which is it made of?

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