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Obtain from first principles the partial derivatives \(\partial f / \partial x\) and \(\partial f / \partial y\) of the function \(f(x, y)\) at the point \((1,2)\), where $$ f(x, y)=2 x^{2}-x y+y^{2} $$

Short Answer

Expert verified
At point (1,2), \( \frac{\partial f}{\partial x} = 2 \) and \( \frac{\partial f}{\partial y} = 3 \).

Step by step solution

01

Understand Partial Derivatives from First Principles

The partial derivative of a function with respect to a variable represents how the function changes as we slightly alter that variable while keeping the other variables constant. From first principles, \( \frac{\partial f}{\partial x} \) at a point \((a, b)\) is given by the limit \( \lim_{h \to 0} \frac{f(a + h, b) - f(a, b)}{h} \) while \( \frac{\partial f}{\partial y} \) is given by \( \lim_{k \to 0} \frac{f(a, b + k) - f(a, b)}{k} \).
02

Calculate \( f(x + h, y) \)

To find \( \frac{\partial f}{\partial x} \), we need \( f(x + h, y) \). Substituting \( x + h \) into the function:\[f(x + h, y) = 2(x + h)^2 - (x + h)y + y^2\].Expanding, we get:\[f(x + h, y) = 2(x^2 + 2xh + h^2) - xy - hy + y^2 = 2x^2 + 4xh + 2h^2 - xy - hy + y^2\].
03

Evaluate the Partial Derivative \( \frac{\partial f}{\partial x} \)

Substituting into the definition of the derivative:\[\frac{\partial f}{\partial x} = \lim_{h \to 0} \frac{f(x + h, y) - f(x, y)}{h} = \lim_{h \to 0} \frac{2x^2 + 4xh + 2h^2 - xy - hy + y^2 - (2x^2 - xy + y^2)}{h}\].Simplifying, cancel out terms:\[= \lim_{h \to 0} \frac{4xh + 2h^2 - hy}{h} = \lim_{h \to 0} (4x + 2h - y)\].As \( h \to 0 \), the derivative becomes \( 4x - y \).
04

Calculate \( f(x, y + k) \)

Next, for \( \frac{\partial f}{\partial y} \), find \( f(x, y + k) \):\[f(x, y + k) = 2x^2 - x(y + k) + (y + k)^2\].Expanding results in:\[f(x, y + k) = 2x^2 - xy - xk + y^2 + 2yk + k^2\].
05

Evaluate the Partial Derivative \( \frac{\partial f}{\partial y} \)

Substitute into the definition for partial derivatives regarding \( y \):\[\frac{\partial f}{\partial y} = \lim_{k \to 0} \frac{f(x, y + k) - f(x, y)}{k} = \lim_{k \to 0} \frac{2x^2 - xy - xk + y^2 + 2yk + k^2 - (2x^2 - xy + y^2)}{k}\].Simplifying, we find:\[= \lim_{k \to 0} \frac{-xk + 2yk + k^2}{k} = \lim_{k \to 0} (-x + 2y + k)\].As \( k \to 0 \), the derivative becomes \( -x + 2y \).
06

Substitute the point \((1, 2)\) into the derivatives

Now that we have the expressions for the partial derivatives, substitute \( x = 1 \) and \( y = 2 \). For \( \frac{\partial f}{\partial x} = 4x - y \):\[4(1) - 2 = 2\].And for \( \frac{\partial f}{\partial y} = -x + 2y \): \[-(1) + 2(2) = 3\].

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Key Concepts

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

First Principles
The method of calculating derivatives from first principles is about getting back to the basics. This approach is foundational for understanding how derivatives, including partial derivatives, truly work. The aim is to comprehend how a function changes with a very small shift in one of its input variables, while maintaining the other inputs constant. In the case of partial derivatives like \( \frac{\partial f}{\partial x} \), you focus on observing infinitesimal changes in the \(x\)-component while keeping \(y\) fixed. It's like observing a reaction to a change if you slightly nudge one aspect while holding others still.

To apply first principles to partial derivatives, consider the specific point in the domain where you're evaluating this change. Use the concept of limits to determine how the function behaves as this shift becomes infinitely small.
Limit Definition
The limit definition of a derivative is a key mathematical tool. It enables us to precisely determine the slope or rate of change at a specific point. When considering the limit definition for partial derivatives, it involves evaluating how the function changes as one input variable approaches zero while others are constant.

For example, to find \( \frac{\partial f}{\partial x} \), you would consider:
  • \( \lim_{h \to 0} \frac{f(a + h, b) - f(a, b)}{h} \)
This expression assesses the change in the function when \(x\) is increased by a tiny amount \(h\) while \(y\) stays at \(b\). Similarly, to determine \( \frac{\partial f}{\partial y} \), you explore:
  • \( \lim_{k \to 0} \frac{f(a, b + k) - f(a, b)}{k} \)
Here, the function's change is observed when \(y\) is tweaked by \(k\), with \(x\) constant.
Derivative Evaluation
Derivative evaluation is the phase where all calculations culminate. You take what you understand about partial derivatives and compute specific values. You plug in your expressions derived from the limit definitions into your known derivatives, simplifying and calculating precisely.

For instance, in the example given with \( f(x, y) = 2x^2 - xy + y^2 \), after determining that \( \frac{\partial f}{\partial x} = 4x - y \) and \( \frac{\partial f}{\partial y} = -x + 2y \), evaluation involves substituting specific values.
  • For the point \((1, 2)\), evaluate \(4(1) - 2 = 2\)
  • For \( -1 + 4 \), you find \(3\)
These values represent the slope of the function surface in the respective directions at \((1, 2)\).
Function Expansion
Function expansion refers to expressing a function at a shifted point in terms of its original point. This concept is crucial for finding derivatives using first principles, as it involves symmetric changes exerted on individual inputs while keeping others unaffected.

In the context of determining \( \frac{\partial f}{\partial x} \), when given the function \(f(x, y)\), you replace \(x\) with \(x + h\) in the whole function expression. Expanding this involves:
  • \( f(x + h, y) = 2(x + h)^2 - (x + h)y + y^2 \)
  • Breaking down: \( = 2x^2 + 4xh + 2h^2 - xy - hy + y^2 \)
  • Simplifying makes it easier to find the limit as \(h\) approaches zero
Similarly, function expansion for \( \frac{\partial f}{\partial y} \) involves replacing \(y\) with \(y + k\) and expanding accordingly.

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Most popular questions from this chapter

Evaluate (a) \(\int_{0}^{8} x^{-1 / 3} \mathrm{~d} x\) (b) \(\int_{3 / 2}^{6} \frac{1}{\sqrt{(2 x-3)}} \mathrm{dx}\) (c) \(\int_{0}^{1} \ln x \mathrm{~d} x\) stating in each case the value of \(x\) for which the integrand becomes unbounded.

A tank has the shape of a cuboid and is open at the top and has a volume of \(4 \mathrm{~m}^{3}\). If the base measurements (in \(\mathrm{m}\) ) are \(x\) by \(y\), show that the surface area (in \(\mathrm{m}^{2}\) ) is given by $$ A=x y+\frac{8}{y}+\frac{8}{x} $$ and find the dimensions of the tank for \(A\) to be a minimum.

Determine which of the following are exact differentials of a function, and find, where appropriate, the corresponding function. (a) \(\left(y^{2}+2 x y+1\right) \mathrm{d} x+\left(2 x y+x^{2}\right) \mathrm{d} y\) (b) \(\left(2 x y^{2}+3 y \cos 3 x\right) \mathrm{d} x+\left(2 x^{2} y+\sin 3 x\right) \mathrm{d} y\) (c) \(\left(6 x y-y^{2}\right) \mathrm{d} x+\left(2 x \mathrm{e}^{y}-x^{2}\right) \mathrm{d} y\) (d) \(\left(z^{3}-3 y\right) \mathrm{d} x+\left(12 y^{2}-3 x\right) \mathrm{d} y+3 x z^{2} \mathrm{~d} z\)

The deflection at the midpoint of a uniform beam of length \(l\), flexural rigidity \(E I\) and weight per unit length \(w\), subject to an axial force \(P\), is $$ d=\frac{w}{m^{2} P}\left(\sec \frac{1}{2} m l-1\right)-\frac{w l^{2}}{8 P} $$ where \(m^{2}=P / E I\). On making the substitution \(\theta=\frac{1}{2} m l\), show that $$ d=\frac{w l^{4}}{32 E I} \frac{2 \sec \theta-2-\theta^{2}}{\theta^{4}} $$ As the force \(P\) is relaxed, the deflection should reduce to that of a beam sagging under its own weight. By first representing \(\sec \theta\) by its Maclaurin series expansion, show that $$ \lim _{\theta \rightarrow 0} d=\frac{5 w l^{4}}{384 E I} $$

Show that $$ f(x, y, z)=x+\frac{x-y}{y-z} $$ satisfies $$ f_{x}+f_{y}+f_{z}=1 $$

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