/*! 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 36 Find the partial derivative of t... [FREE SOLUTION] | 91Ó°ÊÓ

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Find the partial derivative of the function with respect to each variable. $$g(u, v)=v^{2} e^{(2 u / v)}$$

Short Answer

Expert verified
\( \frac{\partial g}{\partial u} = 2v e^{(2u/v)}; \frac{\partial g}{\partial v} = 2(v - u)e^{(2u/v)}.\)

Step by step solution

01

Identify Variables and Expression

The function given is \(g(u, v) = v^2 e^{(2u/v)}\). Our goal is to find the partial derivative with respect to both \(u\) and \(v\).
02

Partial Derivative with Respect to u

To find \( \frac{\partial g}{\partial u} \), treat \(v\) as a constant. The expression \(e^{(2u/v)}\) is an exponential function where \(\frac{2}{v}\) is a constant multiplier. Using the derivative rule for exponential functions, we get:\[ \frac{\partial g}{\partial u} = v^2 \cdot e^{(2u/v)} \cdot \frac{2}{v} \]Simplify:\[ \frac{\partial g}{\partial u} = 2v e^{(2u/v)} \]
03

Partial Derivative with Respect to v

To find \( \frac{\partial g}{\partial v} \), treat \(u\) as a constant. The function is \(v^2 e^{(2u/v)}\), which involves both product and chain rule. Differentiate \(v^2\) and \(e^{(2u/v)}\):- The derivative of \(v^2\) is \(2v\).- The derivative of \(e^{(2u/v)}\) with respect to \(v\) requires the chain rule, giving \( e^{(2u/v)} \cdot \frac{d}{dv}\left(\frac{2u}{v}\right) = -\frac{2u}{v^2} e^{(2u/v)}\).Apply the product rule:\[ \frac{\partial g}{\partial v} = (2v)e^{(2u/v)} + v^2 \left(-\frac{2u}{v^2} e^{(2u/v)}\right) \]Simplify:\[ \frac{\partial g}{\partial v} = 2v e^{(2u/v)} - 2u e^{(2u/v)} = 2(v - u)e^{(2u/v)} \]
04

Conclusion

The partial derivatives are: \[ \frac{\partial g}{\partial u} = 2v e^{(2u/v)} \]\[ \frac{\partial g}{\partial v} = 2(v - u)e^{(2u/v)} \]

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Key Concepts

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

Multivariable Calculus
Multivariable calculus is a branch of mathematics focused on functions with multiple variables. It extends the concepts of calculus, which typically involve a single variable, to spaces with more than one dimension. In the context of functions involving two or more variables, such as \( g(u, v) = v^2 e^{(2u/v)} \), the idea is to explore how these functions change as each variable changes. Think of it as plotting a surface in three dimensions where each point on the surface corresponds to a combination of the variables \( u \) and \( v \).
This branch of calculus involves understanding gradients, which indicate the direction and rate of change of the function, as well as calculating partial derivatives. A partial derivative looks at how a function changes as one variable changes, holding the others constant. This is crucial for optimizing multivariable functions, which has applications in various fields like engineering and economics.
When calculating partial derivatives, it's essential to consider:
  • Each variable independently while treating others as constants.
  • The role of each variable in the function.
This specialized focus helps solve complex problems by systematically studying each variable's impact.
Chain Rule
The chain rule is a fundamental tool in calculus used to differentiate composite functions. It helps determine how changes in input can affect the output, especially when these inputs are functions of other variables. For the function \( g(u, v) = v^2 e^{(2u/v)} \), applying the chain rule is necessary when differentiating \( e^{(2u/v)} \) with respect to \( v \).
The chain rule states that if you have a function \( y = f(g(x)) \), the derivative of \( y \) with respect to \( x \) is the derivative of \( f \) with respect to \( g \) multiplied by the derivative of \( g \) with respect to \( x \). In simpler terms, it breaks down complex differentiations into manageable parts.
In the problem at hand, differentiating \( e^{(2u/v)} \) involves:
  • Recognizing \( e^{(2u/v)} \) as a composite function.
  • Using the chain rule to calculate the derivative of the exponent, \( \frac{2u}{v} \), with respect to \( v \), which yields \( -\frac{2u}{v^2} \).
These steps lead to the derivative \( e^{(2u/v)} \cdot -\frac{2u}{v^2} \), which is crucial for correctly calculating the partial derivative \( \frac{\partial g}{\partial v} \).
Product Rule
The product rule comes into play when differentiating functions that are the product of two or more functions. It is especially useful in multivariable contexts where functions are often intertwined. For the function \( g(u, v) = v^2 e^{(2u/v)} \), the product rule is essential in finding \( \frac{\partial g}{\partial v} \).
According to the product rule, if you have two functions \( f(x) \) and \( g(x) \), the derivative of their product \( f(x)g(x) \) is given by \( f'(x)g(x) + f(x)g'(x) \). Put simply, this rule states that you differentiate each part of the product, one at a time, while treating the other part as constant.
For the problem:
  • Differentiating \( v^2 \) gives \( 2v \).
  • The chain rule helps to differentiate \( e^{(2u/v)} \).
This results in the derivative sum: \( 2v e^{(2u/v)} + v^2(-\frac{2u}{v^2} e^{(2u/v)}) \). Simplifying leads to the expression \( 2(v - u)e^{(2u/v)} \). The product rule allows precise computation of derivatives across products in multivariate settings, enabling easier manipulation and understanding of complex functions.

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Most popular questions from this chapter

Gives a function \(f(x, y)\) and a positive number \(\epsilon\) In each exercise, show that there exists a \(\delta>0\) such that for all \((x, y)\) $$\sqrt{x^{2}+y^{2}}<\delta \Rightarrow|f(x, y)-f(0,0)|<\epsilon$$ $$f(x, y)=y /\left(x^{2}+1\right), \quad \epsilon=0.05$$

Just as you describe curves in the plane parametrically with a pair of equations \(x=f(t), y=g(t)\) defined on some parameter interval \(I\), you can sometimes describe surfaces in space with a triple of equations \(x=f(u, v), y=g(u, v), z=h(u, v)\) defined on some parameter rectangle \(a \leq u \leq b, c \leq v \leq d .\) Many computer algebra systems permit you to plot such surfaces in parametric mode. (Parametrized surfaces are discussed in detail in Section 16.5.) Use a CAS to plot the surfaces in Exercises \(77-80 .\) Also plot several level curves in the \(x y\) -plane. $$\begin{array}{l} x=u \cos v, \quad y=u \sin v, \quad z=u, \quad 0 \leq u \leq 2 \\ 0 \leq v \leq 2 \pi \end{array}$$

If you cannot make any headway with \(\lim _{(x, y) \rightarrow(0,0)} f(x, y)\) in rectangular coordinates, try changing to polar coordinates. Substitute \(x=r \cos \theta, y=r \sin \theta,\) and investigate the limit of the resulting expression as \(r \rightarrow 0 .\) In other words, try to decide whether there exists a number \(L\) satisfying the following criterion: $$|r|<\delta \Rightarrow|f(r, \theta)-L|<\epsilon$$ If such an \(L\) exists, then $$\lim _{(x, y) \rightarrow(0,0)} f(x, y)=\lim _{r \rightarrow 0} f(r \cos \theta, r \sin \theta)=L$$ For instance, $$\lim _{(x, y) \rightarrow(0,0)} \frac{x^{3}}{x^{2}+y^{2}}=\lim _{r \rightarrow 0} \frac{r^{3} \cos ^{3} \theta}{r^{2}}=\lim _{r \rightarrow 0} r \cos ^{3} \theta=0$$ To verify the last of these equalities, we need to show that Equation (1) is satisfied with \(f(r, \theta)=r \cos ^{3} \theta\) and \(L=0 .\) That is, we need to show that given any \(\epsilon>0,\) there exists a \(\delta>0\) such that for all \(r\) and \(\theta\) $$|r|<\delta \Rightarrow\left|r \cos ^{3} \theta-0\right|<\epsilon$$ since $$\left|r \cos ^{3} \theta\right|=|r|\left|\cos ^{3} \theta\right| \leq|r| \cdot 1=|r|$$ the implication holds for all \(r\) and \(\theta\) if we take \(\delta=\epsilon\) In contrast, $$\frac{x^{2}}{x^{2}+y^{2}}=\frac{r^{2} \cos ^{2} \theta}{r^{2}}=\cos ^{2} \theta$$takes on all values from 0 to 1 regardless of how small \(|r|\) is, so that \(\lim _{(x, y) \rightarrow(0,0)} x^{2} /\left(x^{2}+y^{2}\right)\) does not exist. In each of these instances, the existence or nonexistence of the limit as \(r \rightarrow 0\) is fairly clear. Shifting to polar coordinates does not always help, however, and may even tempt us to false conclusions. For example, the limit may exist along every straight line (or ray) \(\theta=\) constant and yet fail to exist in the broader sense. Example 5 illustrates this point. In polar coordinates, \(f(x, y)=\left(2 x^{2} y\right) /\left(x^{4}+y^{2}\right)\) becomes $$f(r \cos \theta, r \sin \theta)=\frac{r \cos \theta \sin 2 \theta}{r^{2} \cos ^{4} \theta+\sin ^{2} \theta}$$for \(r \neq 0 .\) If we hold \(\theta\) constant and let \(r \rightarrow 0,\) the limit is \(0 .\) On the path \(y=x^{2},\) however, we have \(r \sin \theta=r^{2} \cos ^{2} \theta\) and $$\begin{aligned} f(r \cos \theta, r \sin \theta) &=\frac{r \cos \theta \sin 2 \theta}{r^{2} \cos ^{4} \theta+\left(r \cos ^{2} \theta\right)^{2}} \\ &=\frac{2 r \cos ^{2} \theta \sin \theta}{2 r^{2} \cos ^{4} \theta}=\frac{r \sin \theta}{r^{2} \cos ^{2} \theta}=1 \end{aligned}$$ Find the limit of \(f\) as \((x, y) \rightarrow(0,0)\) or show that the limit does not exist. $$f(x, y)=\frac{x^{3}-x y^{2}}{x^{2}+y^{2}}$$

Find the derivative of \(f(x, y)=x^{2}+y^{2}\) in the direction of the unit tangent vector of the curve $$\mathbf{r}(t)=(\cos t+t \sin t) \mathbf{i}+(\sin t-t \cos t) \mathbf{j}, \quad t>0$$

Define \(f(0,0)\) in a way that extends \(f\) to be continuous at the origin. $$f(x, y)=\frac{3 x^{2} y}{x^{2}+y^{2}}$$

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