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If \(z=(x+y) e^{y}\) and \(x=u^{2}+v^{2}\) and \(y=u^{2}-v^{2},\) find the following partial derivatives using the chain rule. Enter your answers as functions of \(u\) and \(v\). \(\frac{\partial z}{\partial u}=\) __________. \(\frac{\partial z}{\partial v}=\) ___________.

Short Answer

Expert verified
The partial derivatives of \(z\) with respect to \(u\) and \(v\) are: \(\frac{\partial z}{\partial u} = 2ue^{(u^2-v^2)}(2u^2+1)\) \(\frac{\partial z}{\partial v} = -2ve^{(u^2-v^2)}(2v^2-1)\)

Step by step solution

01

Write down the given functions and find the required partial derivatives for \(x\) and \(y\)

We are given that: \(x = u^2 + v^2\) \(y = u^2 - v^2\) Therefore, we need to find the partial derivatives \(\frac{\partial x}{\partial u}\), \(\frac{\partial x}{\partial v}\), \(\frac{\partial y}{\partial u}\), and \(\frac{\partial y}{\partial v}\). Now, find the required partial derivatives for \(x\) and \(y\): \(\frac{\partial x}{\partial u} = 2u\) \(\frac{\partial x}{\partial v} = 2v\) \(\frac{\partial y}{\partial u} = 2u\) \(\frac{\partial y}{\partial v} = -2v\)
02

Write down the chain rule for partial derivatives of \(z\) with respect to \(u\) and \(v\)

Next, we'll apply the chain rule to find the partial derivatives of \(z\) with respect to \(u\) and \(v\). The chain rule states that: \(\frac{\partial z}{\partial u} = \frac{\partial z}{\partial x}\cdot\frac{\partial x}{\partial u} + \frac{\partial z}{\partial y}\cdot\frac{\partial y}{\partial u}\) \(\frac{\partial z}{\partial v} = \frac{\partial z}{\partial x}\cdot\frac{\partial x}{\partial v} + \frac{\partial z}{\partial y}\cdot\frac{\partial y}{\partial v}\)
03

Find the partial derivatives of \(z\) with respect to \(x\) and \(y\)

Next, we need to find the partial derivatives \(\frac{\partial z}{\partial x}\) and \(\frac{\partial z}{\partial y}\) given the function \(z = (x+y)e^y\). Using the product rule, we get: \(\frac{\partial z}{\partial x} = e^y (1)\) \(\frac{\partial z}{\partial y} = (x+y)e^y + e^y\) Now, we have all the partial derivatives needed to apply the chain rule for \(\frac{\partial z}{\partial u}\) and \(\frac{\partial z}{\partial v}\).
04

Find the partial derivatives of \(z\) with respect to \(u\) and \(v\)

Now, plug in all the partial derivatives found in Steps 1 and 3 into the chain rule equations from Step 2. \(\frac{\partial z}{\partial u} = e^y(1)\cdot(2u) + [(x+y)e^y + e^y]\cdot(2u)\) \(\frac{\partial z}{\partial v} = e^y(1)\cdot(2v) + [(x+y)e^y + e^y]\cdot(-2v)\) Next, we'll substitute \(x = u^2 + v^2\) and \(y = u^2 - v^2\): \(\frac{\partial z}{\partial u} = e^{(u^2-v^2)}\cdot(2u) + [(u^2+v^2+(u^2-v^2))e^{(u^2-v^2)} + e^{(u^2-v^2)}]\cdot(2u)\) \(\frac{\partial z}{\partial v} = e^{(u^2-v^2)}\cdot(2v) + [(u^2+v^2+(u^2-v^2))e^{(u^2-v^2)} + e^{(u^2-v^2)}]\cdot(-2v)\) Simplifying these expressions, we get: \(\frac{\partial z}{\partial u} = 2ue^{(u^2-v^2)}(2u^2+1)\) \(\frac{\partial z}{\partial v} = -2ve^{(u^2-v^2)}(2v^2-1)\) Therefore, the requested partial derivatives are: \(\frac{\partial z}{\partial u} = 2ue^{(u^2-v^2)}(2u^2+1)\) \(\frac{\partial z}{\partial v} = -2ve^{(u^2-v^2)}(2v^2-1)\)

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Key Concepts

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

Multivariable Calculus
Multivariable calculus extends the concepts of single variable calculus to functions of two or more variables. In this field, we study how to perform operations such as differentiation and integration when there are multiple inputs, and possibly, multiple outputs. Partial derivatives, one of the cornerstones of multivariable calculus, measure how a function changes as only one of the several variables is varied, holding the others constant.

An understanding of multivariable calculus is critical for analyzing real-world scenarios where variables are often not independent, such as in physics (where, for example, position, speed, and acceleration can be functions of multiple spatial variables), economics (considering factors like supply, demand, and time), or any field of engineering involving multidimensional systems. The exercise given demonstrates how multivariable calculus allows us to find tendencies in complex systems where simply 'holding other variables constant' wouldn't suffice.
Chain Rule Application
The chain rule is a fundamental tool in calculus that allows us to compute the derivative of a composite function. When extended to multivariable functions, the chain rule becomes a powerful method to find the rate of change of a function with respect to an external variable by linking the internal variables through their partial derivatives.

In real-life applications, the chain rule can be used to understand the interrelated changes within a system. For instance, in our exercise, by using the chain rule, we determine how a change in the variables 'u' and 'v' affects the function 'z'. This process involves breaking down the problem into smaller, more manageable parts – finding the effect of 'u' and 'v' on 'x' and 'y', then understanding how 'x' and 'y' affect 'z'. The calculated step-by-step solution models the utility of the chain rule in breaking down complex, interdependent systems into calculations based on individual component relationships.
Partial Differentiation
Partial differentiation is the process of finding the derivative of multivariable functions with respect to one variable at a time. It's akin to investigating the effect of slight variations in a single dimension while imagining the rest of the world to be frozen.

For example, in economics, calculating the partial derivative of profit with respect to the price of a single product can tell us how much the profit will change if we only tweak that one price, ignoring other factors. In the context of our exercise, we found partial derivatives of 'z' concerning 'x' and 'y' before applying the chain rule. This allowed us to express the change in 'z' with respect to 'u' and 'v' effectively. Understanding partial differentiation is vital for developing a nuanced appreciation of how multivariate systems evolve along individual axis — it's about pinpointing singular influences within a mesh of variables.

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Most popular questions from this chapter

Given \(F(r, s, t)=r\left(9 s^{4}-t^{5}\right),\) compute: $$F_{r s t}=$$ _________.

In this section we argued that if \(f=f(x, y)\) is a function of two variables and if \(f_{x}\) and \(f_{y}\) both exist and are continuous in an open disk containing the point \(\left(x_{0}, y_{0}\right),\) then \(f\) is differentiable at \(\left(x_{0}, y_{0}\right) .\) This condition ensures that \(f\) is differentiable at \(\left(x_{0}, y_{0}\right),\) but it does not define what it means for \(f\) to be differentiable at \(\left(x_{0}, y_{0}\right) .\) In this exercise we explore the definition of differentiability of a function of two variables in more detail. Throughout, let \(g\) be the function defined by \(g(x, y)=\sqrt{|x y|}\) a. Use appropriate technology to plot the graph of \(g\) on the domain \([-1,1] \times[-1,1] .\) Explain why \(g\) is not locally linear at (0,0) b. Show that both \(g_{x}(0,0)\) and \(g_{y}(0,0)\) exist. If \(g\) is locally linear at \((0,0),\) what must be the equation of the tangent plane \(L\) to \(g\) at (0,0)\(?\) c. Recall that if a function \(f=f(x)\) of a single variable is differentiable at \(x=x_{0},\) then $$f^{\prime}\left(x_{0}\right)=\lim _{h \rightarrow 0} \frac{f\left(x_{0}+h\right)-f\left(x_{0}\right)}{h}$$ exists. We saw in single variable calculus that the existence of \(f^{\prime}\left(x_{0}\right)\) means that the graph of \(f\) is locally linear at \(x=x_{0}\). In other words, the graph of \(f\) looks like its linearization \(L(x)=f\left(x_{0}\right)+\) \(f^{\prime}\left(x_{0}\right)\left(x-x_{0}\right)\) for \(x\) close to \(x_{0} .\) That is, the values of \(f(x)\) can be closely approximated by \(L(x)\) as long as \(x\) is close to \(x_{0}\). We can measure how good the approximation of \(L(x)\) is to \(f(x)\) with the error function $$E(x)=L(x)-f(x)=f\left(x_{0}\right)+f^{\prime}\left(x_{0}\right)\left(x-x_{0}\right)-f(x)$$ As \(x\) approaches \(x_{0}, E(x)\) approaches \(f\left(x_{0}\right)+f^{\prime}\left(x_{0}\right)(0)-f\left(x_{0}\right)=0\), and so \(L(x)\) provides increasingly better approximations to \(f(x)\) as \(x\) gets closer to \(x_{0} .\) Show that, even though \(g(x, y)=\sqrt{|x y|}\) is not locally linear at \((0,0),\) its error term $$ E(x, y)=L(x, y)-g(x, y) $$ at (0,0) has a limit of 0 as \((x, y)\) approaches \((0,0) .\) (Use the linearization you found in part (b).) This shows that just because an error term goes to 0 as \((x, y)\) approaches \(\left(x_{0}, y_{0}\right),\) we cannot conclude that a function is locally linear at \(\left(x_{0}, y_{0}\right)\). d. As the previous part illustrates, having the error term go to 0 does not ensure that a function of two variables is locally linear. Instead, we need a notation of a relative error. To see how this works, let us return to the single variable case for a moment and consider \(f=f(x)\) as a function of one variable. If we let \(x=x_{0}+h,\) where \(|h|\) is the distance from \(x\) to \(x_{0}\), then the relative error in approximating \(f\left(x_{0}+h\right)\) with \(L\left(x_{0}+h\right)\) is $$\frac{E\left(x_{0}+h\right)}{h}$$ Show that, for a function \(f=f(x)\) of a single variable, the limit of the relative error is 0 as \(h\) approaches 0 . e. Even though the error term for a function of two variables might have a limit of 0 at a point, our example shows that the function may not be locally linear at that point. So we use the concept of relative error to define differentiability of a function of two variables. When we consider differentiability of a function \(f=f(x, y)\) at a point \(\left(x_{0}, y_{0}\right),\) then if \(x=x_{0}+h\) and \(y=y_{0}+k,\) the distance from \((x, y)\) to \(\left(x_{0}, y_{0}\right)\) is \(\sqrt{h^{2}+k^{2}}\)

Suppose that \(T=x^{2}+y^{2}-2 z\) where $$\begin{array}{l}x=\rho \sin (\phi) \cos (\theta) \\\y=\rho \sin (\phi) \sin (\theta) \\\z=\rho \cos (\phi)\end{array}$$ a. Construct a tree diagram representing the dependencies among the variables. b. Apply the chain rule to find the partial derivatives $$\frac{\partial T}{\partial \rho}, \frac{\partial T}{\partial \phi}, \text { and } \frac{\partial T}{\partial \theta} .$$

If a continuous function \(f\) of a single variable has exactly one critical number with a relative maximum at that critical point, then the value of \(f\) at that critical point is an absolute maximum. In this exercise we see that the same is not always true for functions of two variables. Let \(f(x, y)=3 x e^{y}-x^{3}-e^{3 y}\) (from "' The Only Critical Point in Town"" Test by Ira Rosenholz and Lowell Smylie in the Mathematics Magazine, VOL 58 NO 3 May \(1985 .\) ). Show that \(f\) has exactly one critical point, has a relative maximum value at that critical point, but that \(f\) has no absolute maximum value. Use appropriate technology to draw the surface defined by \(f\) to see graphically how this happens.

The airlines place restrictions on luggage that can be carried onto planes. \- A carry-on bag can weigh no more than 40 lbs. \- The length plus width plus height of a bag cannot exceed 45 inches. \- The bag must fit in an overhead bin. Let \(x, y,\) and \(z\) be the length, width, and height (in inches) of a carry on bag. In this problem we find the dimensions of the bag of largest volume, \(V=x y z,\) that satisfies the second restriction. Assume that we use all 45 inches to get a maximum volume. (Note that this bag of maximum volume might not satisfy the third restriction.) a. Write the volume \(V=V(x, y)\) as a function of just the two variables \(x\) and \(y\) b. Explain why the domain over which \(V\) is defined is the triangular region \(R\) with vertices \((0,0),(45,0),\) and (0,45) . c. Find the critical points, if any, of \(V\) in the interior of the region \(R\). d. Find the maximum value of \(V\) on the boundary of the region \(R\), and then determine the dimensions of a bag with maximum volume on the entire region \(R\). (Note that most carry-on bags sold today measure 22 by 14 by 9 inches with a volume of 2772 cubic inches, so that the bags will fit into the overhead bins.)

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