Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

A ball bearing manufacturing plant is using air to cool chromium steel balls \((k=40 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\). The convection heat transfer coefficient for the cooling is determined experimentally as a function of air velocity to be \(h=18.05 \mathrm{~V}^{0.56}\), where \(h\) and \(V\) are in \(\mathrm{W} / \mathrm{m}^{2}, \mathrm{~K}\) and $\mathrm{m} / \mathrm{s}$, respectively. At a given moment during the cooling process with the air temperature at \(5^{\circ} \mathrm{C}\), a chromium steel ball has a surface temperature of \(450^{\circ} \mathrm{C}\). Using appropriate software, determine the effect of the air velocity \((V)\) on the temperature gradient in the chromium steel ball at the surface. By varying the air velocity from \(0.2\) to \(2.4 \mathrm{~m} / \mathrm{s}\) with increments of $0.2 \mathrm{~m} / \mathrm{s}$, plot the temperature gradient in the chromium steel ball at the surface as a function of air velocity.

Short Answer

Expert verified
Answer: The temperature gradient in a chromium steel ball at the surface is affected by air velocity. As air velocity increases, the convection heat transfer coefficient also increases, leading to a higher rate of heat transfer by convection. This results in an increase in the temperature gradient within the steel ball at the surface. To determine the relationship between air velocity and temperature gradient, we can follow the steps discussed in the solution and plot the temperature gradient as a function of air velocity.

Step by step solution

01

Find the Convection Heat Transfer Coefficient using the given function

For air velocity \(V\), the convection heat transfer coefficient \(h\) is given by the equation: \(h = 18.05V^{0.56}\).
02

Apply Fourier's Law of Heat Conduction

Fourier's law states that the rate of heat conduction (\(\dot{Q}\)) is proportional to the temperature gradient (\(\frac{dT}{dx}\)). The equation is: \(\dot{Q} = -k\frac{dT}{dx}\), where \(k\) is the thermal conductivity.
03

Apply Newton's Law of Cooling

Newton's law states that the rate of heat transfer by convection is proportional to the temperature difference between the surface temperature (\(T_s\)) and the air temperature (\(T_\infty\)). The equation is: \(\dot{Q} = h(T_s - T_\infty)\).
04

Equate the rates of heat conduction and heat transfer by convection

Since the rate of heat conduction is equal to the rate of heat transfer by convection, we have: \(-k\frac{dT}{dx} = h(T_s - T_\infty)\)
05

Calculate the temperature gradient

First, isolate the temperature gradient term in the equation: \(\frac{dT}{dx} = -\frac{h}{k}(T_s - T_\infty)\) Now, we can calculate the temperature gradient for different air velocities (\(V\)) from \(0.2 \mathrm{~m/s}\) to \(2.4 \mathrm{~m/s}\) with increments of \(0.2 \mathrm{~m/s}\), using the given values of \(T_s = 450^{\circ} \mathrm{C}\), \(T_\infty = 5^{\circ} \mathrm{C}\), and \(k = 40 \mathrm{~W/m\cdot K}\).
06

Plot the temperature gradient as a function of air velocity

Using appropriate software (such as Excel, Python, or MATLAB), plot the temperature gradient in the chromium steel ball at the surface as a function of air velocity. Each point on the graph will represent the corresponding temperature gradient for the given air velocity. In conclusion, by following these steps, we can determine the effect of air velocity on the temperature gradient in the chromium steel ball at the surface, and visualize the relationship through a plot.

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 Vaia!

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

Consider fluid flowing with a free stream velocity of $1 \mathrm{ft} / \mathrm{s}\( over a flat plate, where the critical Reynolds number is \)5 \times 10^{5}$. Determine the distance from the leading edge at which the transition from laminar to turbulent flow occurs for air (at 1 atm), liquid water, isobutane, and engine oil, and mercury. Evaluate all properties at $50^{\circ} \mathrm{F}$.

Using a cylinder, a sphere, and a cube as examples, show that the rate of heat transfer is inversely proportional to the nominal size of the object. That is, heat transfer per unit area increases as the size of the object decreases.

In any forced or natural convection situation, the velocity of the flowing fluid is zero where the fluid wets any stationary surface. The magnitude of heat flux where the fluid wets a stationary surface is given by (a) \(k\left(T_{\text {fluid }}-T_{\text {wall }}\right)\) (b) \(\left.k \frac{d T}{d y}\right|_{\text {wall }}\) (c) \(\left.k \frac{d^{2} T}{d y^{2}}\right|_{\text {wall }}\) (d) \(\left.h \frac{d T}{d y}\right|_{\text {wall }}\) (e) None of them

How is the modified Reynolds analogy expressed? What is the value of it? What are its limitations?

In turbulent flow, one can estimate the Nusselt number using the analogy between heat and momentum transfer (Colburn analogy). This analogy relates the Nusselt number to the coefficient of friction, \(C_{p}\) as (a) \(\mathrm{Nu}=0.5 C_{f} \operatorname{Re} \mathrm{Pr}^{1 / 3}\) (c) \(\mathrm{Nu}=C_{f} \operatorname{Re} \mathrm{Pr}^{1 / 3}\) (e) \(\mathrm{Nu}=C_{f} \operatorname{Re}^{1 / 2} \operatorname{Pr}^{1 / 3}\) (d) \(\mathrm{Nu}=C_{f} \operatorname{Re} P r^{2 / 3}\)

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.

Sign-up for free