/*! 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 27 $$ \text { Given } u=\sin \fra... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

$$ \text { Given } u=\sin \frac{r}{t}+\ln \frac{t}{r} . \text { Verify } t \frac{\partial u}{\partial t}+r \frac{\partial u}{\partial r}=0 $$.

Short Answer

Expert verified
\( t \frac{\partial u}{\partial t} + r \frac{\partial u}{\partial r} = 0 \) is verified.

Step by step solution

01

Compute the partial derivative of \( u \) with respect to \( t \)

Given that \[ u = \sin \left(\frac{r}{t}\right) + \ln \left(\frac{t}{r}\right) \]First, use the chain rule to find \( \frac{\partial u}{\partial t} \).The partial derivative of \( \sin \left(\frac{r}{t}\right) \) with respect to \( t \) is:\[ \frac{\partial}{\partial t} \left( \sin \left(\frac{r}{t}\right) \right) = \cos \left(\frac{r}{t}\right) \cdot \left(-\frac{r}{t^2}\right) = -\frac{r \cos \left(\frac{r}{t}\right)}{t^2} \]The partial derivative of \( \ln \left(\frac{t}{r}\right) \) with respect to \( t \) is:\[ \frac{\partial}{\partial t} \left(\ln \left(\frac{t}{r}\right)\right) = \frac{1}{t} \]Combining these, we get:\[ \frac{\partial u}{\partial t} = -\frac{r \cos \left(\frac{r}{t}\right)}{t^2} + \frac{1}{t} \]
02

Compute the partial derivative of \( u \) with respect to \( r \)

Next, use the chain rule to find \( \frac{\partial u}{\partial r} \).The partial derivative of \( \sin \left(\frac{r}{t}\right) \) with respect to \( r \) is:\[ \frac{\partial}{\partial r} \left( \sin \left(\frac{r}{t}\right) \right) = \cos \left(\frac{r}{t}\right) \cdot \left(\frac{1}{t}\right) = \frac{\cos \left(\frac{r}{t}\right)}{t} \]The partial derivative of \( \ln \left(\frac{t}{r}\right) \) with respect to \( r \) is:\[ \frac{\partial}{\partial r} \left(\ln \left(\frac{t}{r}\right)\right) = -\frac{1}{r} \]Combining these, we get:\[ \frac{\partial u}{\partial r} = \frac{\cos \left(\frac{r}{t}\right)}{t} - \frac{1}{r} \]
03

Verify \( t \frac{\partial u}{\partial t} + r \frac{\partial u}{\partial r} = 0 \)

Substitute \( \frac{\partial u}{\partial t} \) and \( \frac{\partial u}{\partial r} \) into the expression:\[ t \cdot \left( -\frac{r \cos \left(\frac{r}{t}\right)}{t^2} + \frac{1}{t} \right) + r \cdot \left( \frac{\cos \left(\frac{r}{t}\right)}{t} - \frac{1}{r} \right) \]Simplifying, we get:\[ t \left( -\frac{r \cos \left(\frac{r}{t}\right)}{t^2} + \frac{1}{t} \right) + r \left( \frac{\cos \left(\frac{r}{t}\right)}{t} - \frac{1}{r} \right) \]This simplifies to:\[ -\frac{r \cos \left(\frac{r}{t}\right)}{t} + 1 + \frac{r \cos \left(\frac{r}{t}\right)}{t} - 1 = 0 \]Therefore, the expression is verified:\[ t \frac{\partial u}{\partial t} + r \frac{\partial u}{\partial r} = 0 \]

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.

partial derivatives
Partial derivatives are a fundamental concept in calculus, especially in multivariable functions. They indicate how a function changes as one specific variable changes while keeping other variables constant. For instance, in the given exercise, the function \(u\) is defined in terms of two variables, \(r\) and \(t\). By computing the partial derivatives \(\frac{\partial u}{\partial t}\) and \(\frac{\partial u}{\partial r}\), we understand how \(u\) varies with each variable independently.

Here’s a summary of the partial derivatives we computed in the exercise:
  • The partial derivative of \(\sin \left(\frac{r}{t}\right)\) with respect to \(t\): \( -\frac{r \cos \left(\frac{r}{t}\right)}{t^2} \)
  • The partial derivative of \( \ln \left(\frac{t}{r}\right) \) with respect to \( t \): \( \frac{1}{t} \)

Combining both, we have: \( \frac{\partial u}{\partial t} = -\frac{r \cos \left(\frac{r}{t}\right)}{t^2} + \frac{1}{t} \).

Similarly for the variable \( r \):
  • The partial derivative of \( \sin \left(\frac{r}{t}\right) \) with respect to \( r \): \( \frac{\cos \left(\frac{r}{t}\right)}{t} \)
  • The partial derivative of \( \ln \left(\frac{t}{r}\right) \) with respect to \( r \): \( -\frac{1}{r} \)

Combining both, we have: \( \frac{\partial u}{\partial r} = \frac{\cos \left(\frac{r}{t}\right)}{t} - \frac{1}{r} \).

This step-by-step process allows us to isolate the influence of each variable, making it easier to analyze multivariable functions.
chain rule
The chain rule is a powerful tool in calculus that helps us find the derivative of composite functions. In simpler terms, it allows us to differentiate functions nested within other functions. When applying the chain rule to partial derivatives, we need to take care of each layer of the function separately.

In the given exercise, the chain rule is crucial for finding derivatives for terms like \( \sin \left(\frac{r}{t}\right)\). Here’s an illustration:
  • For \( \frac{\partial}{\partial t} \left( \sin \left(\frac{r}{t}\right) \right)\),
    treat \( \frac{r}{t} \) as a single entity. The outer function is the sine function, and its derivative is the cosine function. This gives us \( \cos \left(\frac{r}{t}\right) \).
  • Next, handle the inner function \( \frac{r}{t} \). The derivative with respect to \( t \) is \( -\frac{r}{t^2} \).
  • Combining these by the chain rule, we get: \( \cos \left(\frac{r}{t}\right) \cdot \left( -\frac{r}{t^2} \right) = -\frac{r \cos \left(\frac{r}{t}\right)}{t^2} \).


Similar steps are followed for other terms, ensuring we correctly differentiate the nested functions. Understanding and properly applying the chain rule is pivotal for tackling more complex differentiation problems.
simplification of expressions
Simplification of expressions is the process of condensing complex mathematical statements into their simplest form. This makes them easier to work with and understand, especially in multi-step problems.

Let's look at how we simplified expressions in the final step of the given exercise:
  • Start by substituting the partial derivatives back into the expression \( t \frac{\partial u}{\partial t} + r \frac{\partial u}{\partial r} \).
  • The substitution leads to: \[ t \cdot \left( -\frac{r \cos \left(\frac{r}{t}\right)}{t^2} + \frac{1}{t} \right) + r \cdot \left( \frac{\cos \left(\frac{r}{t}\right)}{t} - \frac{1}{r} \right) \]
  • .

  • Distribute \( t \) and \( r \) in the respective terms: \[ t \left( -\frac{r \cos \left(\frac{r}{t}\right)}{t^2} + \frac{1}{t} \right) + r \left( \frac{\cos \left(\frac{r}{t}\right)}{t} - \frac{1}{r} \right) \]

  • Simplify each term individually: \[ -\frac{r \cos \left(\frac{r}{t}\right)}{t} + 1 + \frac{r \cos \left(\frac{r}{t}\right)}{t} - 1 \]

  • Notice that \( -\frac{r \cos \left(\frac{r}{t}\right)}{t} \) and \( \frac{r \cos \left(\frac{r}{t}\right)}{t} \) cancel each other out, leaving \( 1 - 1 \), which simplifies to 0.


This final verification step shows us that: \( t \frac{\partial u}{\partial t} + r \frac{\partial u}{\partial r} = 0 \). Simplification brings clarity, making complex equations more manageable and confirming our solution's accuracy.

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

Water is flowing into a tank in the form of a right-circular cylinder at the rate of \(\frac{4}{5} \pi \mathrm{ft}^{3} / \mathrm{min}\). The tank is stretching in such a way that even though it remains cylindrical, its radius is increasing at the rate of \(0.002 \mathrm{ft} / \mathrm{min}\). How fast is the surface of the water rising when the radius is \(2 \mathrm{ft}\) and the volume of water in the tank is \(20 \pi \mathrm{ft}^{3}\) ?

At a given instant, the length of one leg of a right triangle is \(10 \mathrm{ft}\) and it is increasing at the rate of \(1 \mathrm{ft} / \mathrm{min}\) and the length of the other leg of the right triangle is \(12 \mathrm{ft}\) and it is decreasing at the rate of \(2 \mathrm{ft} / \mathrm{min}\). Find the rate of change of the measure of the acute angle opposite the leg of length \(12 \mathrm{ft}\) at the given instant.

In Exercises 15 through 18, show that \(u(x, y)\) satisfies the equation $$ \frac{\partial^{2} u}{\partial x^{2}}+\frac{\partial^{2} u}{\partial y^{2}}=0 $$ which is known as Laplace's equation in \(R^{2}\). $$ u(x, y)=e^{x} \sin y+e^{y} \cos x $$

The specific gravity \(s\) of an object is given by the formula $$ s=\frac{A}{A-W} $$ where \(A\) is the number of pounds in the weight of the object in air and \(W\) is the number of pounds in the weight of the object in water. If the weight of an object in air is read as \(20 \mathrm{lb}\) with a possible error of \(0.01 \mathrm{lb}\) and its weight in water is read as \(12 \mathrm{lb}\) with a possible error of \(0.02 \mathrm{lb}\), find approximately the largest possible error in calculating \(s\) from these measurements. Also find the largest possible relative error.

If \(f(x, y)=x y e^{x y}, \Delta x=-0.1\), and \(\Delta y=0.2\), find (a) the increment of \(f\) at \((2,-4)\) and (b) the total differential of \(f\) at \((2,-4)\).

See all solutions

Recommended explanations on Math 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.