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Use the method of your choice to ate the following limits. $$\lim _{(x, y) \rightarrow(1,1)} \frac{x^{2}+x y-2 y^{2}}{2 x^{2}-x y-y^{2}}$$

Short Answer

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#tag_title# Step 2: Simplify the Expression #tag_content# Now let's simplify the expression inside the limit: $$\lim_{u \rightarrow 0} \frac{y^2 + 2uy + u^2 + y^2 + uy - 2y^2}{2y^2 + 4uy + 2u^2 - y^2 - uy - y^2}$$ $$\lim_{u \rightarrow 0} \frac{u^2 + 2uy}{2u^2 + 4uy - y^2}$$ Now that the expression is simplified, we can proceed to calculate the limit as `u` approaches `0`. #tag_title# Step 3: Evaluate the Limit #tag_content# As `u` approaches `0`, the expression becomes: $$\lim_{u \rightarrow 0} \frac{0^2 + 2(0)y}{2(0)^2 + 4(0)y - y^2} = \frac{0}{-y^2} = 0$$ Thus, the limit of the function as `(x, y)` approaches `(1, 1)` is `0`.

Step by step solution

01

Substitution

Let's use the substitution `u = x - y`. Then, we rewrite the expression in terms of `u`: $$\lim_{(x, y) \rightarrow (1, 1)} \frac{x^2 + xy - 2y^2}{2x^2 - xy - y^2} = \lim_{u \rightarrow 0} \frac{(y + u)^2 + (y + u)y - 2y^2}{2(y + u)^2 - (y + u)y - y^2}$$

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Key Concepts

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

Limits
The concept of limits is a fundamental aspect of calculus. It helps us understand how a function behaves as it approaches a certain point. Limits allow us to evaluate functions that might seem difficult to define or approach values at particular points where they are not directly computable. This can be especially useful in cases involving indeterminate forms like 0/0.

When dealing with two-variable limits, the approach is slightly different. Here, we consider the behavior of the function as both input variables approach specific values. It's important to check if the limit is the same regardless of the path taken to reach that point. Imagine approaching from different directions like along the x-axis, y-axis, or diagonal. Consistency across paths indicates a well-defined limit.

In the exercise provided, the goal is to find the limit of a multivariable expression as \((x, y)\) approaches \((1, 1)\). This involves checking if the limit is the same from various paths, which requires a thorough analysis.
Multivariable functions
Multivariable functions extend the notion of single-variable functions into higher dimensions. Instead of a function with one input and one output, we have functions with multiple inputs and potentially multiple outputs. In mathematical terms, a function \(f(x, y)\) maps pairs of inputs \((x, y)\) to an output value.

Analyzing these functions involves understanding how changes in one variable affect the overall function. It becomes slightly more complex than single-variable calculus since it involves dealing with partial derivatives and gradients. However, the essential tactics remain the same: observe and analyze the behavior of the function as coordinates change.

The exercise at hand considers a function defined by a rational expression in terms of \(x\) and \(y\). The objective is to evaluate this function's behavior as both \(x\) and \(y\) simultaneously approach \(1\). It's crucial to manage each variable's effect on the function, which in this case requires a clever substitution to simplify the problem.
Substitution method
The substitution method is a technique often used in calculus to simplify problems involving limits. The main idea is to replace variables or expressions with easier terms. This can help transform a complex expression into a more manageable one.

In the context of the given problem, using the substitution \(u = x - y\), we transform the multivariable limit problem into a simpler task. This substitution helps to evaluate the original limit by expressing it as a limit of a single variable \(u\).
  • The original expression is changed to depend only on \(u\) by rewriting \(x = y + u\).
  • The limit then becomes easier to handle since \(u\) tends to 0 as \((x, y)\) approaches \((1, 1)\).

This strategy is incredibly useful when direct evaluation does not yield obvious results or when simplification is necessary to eliminate indeterminate forms.

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Most popular questions from this chapter

Maximizing a sum Geometric and arithmetic means Prove that the geometric mean of a set of positive numbers \(\left(x_{1} x_{2} \cdots x_{n}\right)^{1 / n}\) is no greater than the arithmetic mean \(\left(x_{1}+\cdots+x_{n}\right) / n\) in the following cases. a. Find the maximum value of \(x y z,\) subject to \(x+y+z=k\) where \(k\) is a real number and \(x>0, y>0,\) and \(z>0 .\) Use the result to prove that $$(x y z)^{1 / 3} \leq \frac{x+y+z}{3}$$ b. Generalize part (a) and show that $$\left(x_{1} x_{2} \cdots x_{n}\right)^{1 / n} \leq \frac{x_{1}+\cdots+x_{n}}{n}$$

Show that if \(f(x, y)=\frac{a x+b y}{c x+d y},\) where \(a, b, c,\) and \(d\) are real numbers with \(a d-b c=0,\) then \(f_{x}=f_{y}=0,\) for all \(x\) and \(y\) in the domain of \(f\). Give an explanation.

Find the points (if they exist) at which the following planes and curves intersect. $$8 x+15 y+3 z=20 ; \quad \mathbf{r}(t)=\langle 1, \sqrt{t},-t\rangle, \text { for } t>0$$

Ideal Gas Law Many gases can be modeled by the Ideal Gas Law, \(P V=n R T,\) which relates the temperature \((T,\) measured in Kelvin (K)), pressure ( \(P\), measured in Pascals (Pa)), and volume ( \(V\), measured in \(\mathrm{m}^{3}\) ) of a gas. Assume that the quantity of gas in question is \(n=1\) mole (mol). The gas constant has a value of \(R=8.3 \mathrm{m}^{3} \cdot \mathrm{Pa} / \mathrm{mol} \cdot \mathrm{K}.\) a. Consider \(T\) to be the dependent variable and plot several level curves (called isotherms) of the temperature surface in the region \(0 \leq P \leq 100,000\) and \(0 \leq V \leq 0.5.\) b. Consider \(P\) to be the dependent variable and plot several level curves (called isobars) of the pressure surface in the region \(0 \leq T \leq 900\) and \(0< V \leq 0.5.\) c. Consider \(V\) to be the dependent variable and plot several level curves of the volume surface in the region \(0 \leq T \leq 900\) and \(0 < P \leq 100,000.\)

The flow of heat along a thin conducting bar is governed by the one- dimensional heat equation (with analogs for thin plates in two dimensions and for solids in three dimensions) $$\frac{\partial u}{\partial t}=k \frac{\partial^{2} u}{\partial x^{2}},$$ where \(u\) is a measure of the temperature at a location \(x\) on the bar at time t and the positive constant \(k\) is related to the conductivity of the material. Show that the following functions satisfy the heat equation with \(k=1.\) \(u(x, t)=A e^{-a^{2} t} \cos a x,\) for any real numbers \(a\) and \(A\)

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