Chapter 4: Problem 4
Find the two-variable Maclaurin series for the following functions. $$e^{x y}$$
Short Answer
Expert verified
The Maclaurin series for \(e^{xy}\) is \(1 + xy\).
Step by step solution
01
Understand the Maclaurin Series
The Maclaurin series is a special case of the Taylor series, centered at 0. For a function of two variables, the Maclaurin series expansion is given by: \[ f(x,y) = f(0,0) + \frac{1}{1!}(f_x(0,0)x + f_y(0,0)y) + \frac{1}{2!}(f_{xx}(0,0)x^2 + 2f_{xy}(0,0)xy + f_{yy}(0,0)y^2) + \ \text{higher order terms} \] where \( f_x, f_y, f_{xx}, f_{xy}, f_{yy} \) are the partial derivatives of \( f \).
02
Calculate the Function Value at (0,0)
Evaluate \( f(0,0) \) for \( f(x,y) = e^{xy} \): \[ f(0,0) = e^{0 \times 0} = e^0 = 1 \]
03
Calculate the First Order Partial Derivatives
Find the first order partial derivatives \( f_x \) and \( f_y \): \[ f_x = \frac{\partial}{\partial x} e^{xy} = y e^{xy} \ f_y = \frac{\partial}{\partial y} e^{xy} = x e^{xy} \] Evaluate at the origin (0,0): \( f_x(0,0) = y e^{0} = 0 \) \( f_y(0,0) = x e^{0} = 0 \)
04
Calculate the Second Order Partial Derivatives
Find the second order partial derivatives \( f_{xx}, f_{xy} \) and \( f_{yy} \): \[ f_{xx} = \frac{\partial^2}{\partial x^2} e^{xy} = y^2 e^{xy} \ f_{xy} = \frac{\partial^2}{\partial x \partial y} e^{xy} = (1 + xy) e^{xy} \ f_{yy} = \frac{\partial^2}{\partial y^2} e^{xy} = x^2 e^{xy} \] Evaluate at the origin (0,0): \( f_{xx}(0,0) = y^2 e^0 = 0 \) \( f_{xy}(0,0) = 1 \times e^0 = 1 \) \( f_{yy}(0,0) = x^2 e^0 = 0 \)
05
Assemble the Maclaurin Series
Using the partial derivatives, construct the Maclaurin series: \[ f(x,y) = 1 + 0 \times x + 0 \times y + \frac{1}{2!}(0 \times x^2 + 2 \times 1 \times xy + 0 \times y^2) \ = 1 + xy \]
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
two-variable functions
A two-variable function involves two inputs, usually represented as \(x\) and \(y\), which produce a single output. Unlike single-variable functions, which map one input to one output, two-variable functions map a pair of inputs to one output. This type of function can be represented as \(f(x, y)\). For example, the function \(f(x, y) = e^{xy}\) takes two variables, \(x\) and \(y\), and calculates the output by raising the natural exponential constant \(e\) to the power of \(xy\).
This nature of having two variables allows us to create 3D plots where the surface height represents the output of the function for every pair of \(x\) and \(y\) values.
The more complex structure of two-variable functions makes techniques like partial derivatives and expansions even more essential in analyzing and understanding them.
This nature of having two variables allows us to create 3D plots where the surface height represents the output of the function for every pair of \(x\) and \(y\) values.
The more complex structure of two-variable functions makes techniques like partial derivatives and expansions even more essential in analyzing and understanding them.
partial derivatives
Partial derivatives measure how a function changes as one of its input variables changes while keeping the other constant. For a two-variable function like \(f(x, y)\), partial derivatives are denoted as \(f_x\) (the derivative with respect to \(x\)) and \(f_y\) (the derivative with respect to \(y\)).
To compute \(f_x\), treat \(y\) as a constant and differentiate with respect to \(x\). Conversely, to get \(f_y\), treat \(x\) as a constant and differentiate with respect to \(y\).
For \(f(x, y) = e^{xy}\), the partial derivatives are:
To compute \(f_x\), treat \(y\) as a constant and differentiate with respect to \(x\). Conversely, to get \(f_y\), treat \(x\) as a constant and differentiate with respect to \(y\).
For \(f(x, y) = e^{xy}\), the partial derivatives are:
- \(f_x = \frac{\partial}{\backslash\text {partial x}} e^{xy} = ye^{xy}\)
- \(f_y = \frac{\partial}{\partial y} e^{xy} = xe^{xy}\)
Taylor series expansion
The Taylor series expansion approximates functions using infinite sums of their derivatives at a specific point. For a function of a single variable, it's written as:
\[f(x) = f(a) + f'(a)(x – a) + \frac{f''(a)}{2!}(x – a)^2 + \frac{f'''(a)}{3!}(x – a)^3 + \text{...}\]
For a two-variable function, a similar expansion can be done. The Maclaurin series is a special case of the Taylor series centered at \(x = 0\) and \(y = 0\). The Maclaurin series for a function \(f(x, y)\) is given by:
\[f(x,y) = f(0,0) + \frac{1}{1!}(f_x(0,0)x + f_y(0,0)y) + \frac{1}{2!}(f_{xx}(0,0)x^2 + 2f_{xy}(0,0)xy + f_{yy}(0,0)y^2) + \text{higher order terms}\]
This formula uses partial derivatives evaluated at the origin to build the series. In our example, for \(f(x, y) = e^{xy}\), the series expansion simplifies to \(1 + xy\). This shows how useful Taylor series expansions can be in approximating function behaviors using polynomials.
\[f(x) = f(a) + f'(a)(x – a) + \frac{f''(a)}{2!}(x – a)^2 + \frac{f'''(a)}{3!}(x – a)^3 + \text{...}\]
For a two-variable function, a similar expansion can be done. The Maclaurin series is a special case of the Taylor series centered at \(x = 0\) and \(y = 0\). The Maclaurin series for a function \(f(x, y)\) is given by:
\[f(x,y) = f(0,0) + \frac{1}{1!}(f_x(0,0)x + f_y(0,0)y) + \frac{1}{2!}(f_{xx}(0,0)x^2 + 2f_{xy}(0,0)xy + f_{yy}(0,0)y^2) + \text{higher order terms}\]
This formula uses partial derivatives evaluated at the origin to build the series. In our example, for \(f(x, y) = e^{xy}\), the series expansion simplifies to \(1 + xy\). This shows how useful Taylor series expansions can be in approximating function behaviors using polynomials.
second order partial derivatives
Second order partial derivatives are the derivatives of the first order partial derivatives. They help to understand the curvature of the function. For a two-variable function \(f(x, y)\), these include:
For \(f(x, y) = e^{xy}\), these second order partial derivatives are:
Evaluating at \((0, 0)\), we get:
These second order partial derivatives are used to construct the higher order terms in the Maclaurin series.
- \(f_{xx}\) – The second partial derivative with respect to \(x\)
- \(f_{yy}\) – The second partial derivative with respect to \(y\)
- \(f_{xy}\) and \(f_{yx}\) – Mixed partial derivatives, representing the change first with respect to one variable and then the other
For \(f(x, y) = e^{xy}\), these second order partial derivatives are:
- \(f_{xx} = \frac{\partial^2}{\partial x^2} e^{xy} = y^2 e^{xy}\)
- \(f_{xy} = \frac{\partial^2}{\partial x \partial y} e^{xy} = (1 + xy)e^{xy}\)
- \(f_{yy} = \frac{\partial^2}{\partial y^2} e^{xy} = x^2 e^{xy}\)
Evaluating at \((0, 0)\), we get:
- \(f_{xx}(0,0) = 0\)
- \(f_{xy}(0, 0) = 1\)
- \(f_{yy}(0,0) = 0\)
These second order partial derivatives are used to construct the higher order terms in the Maclaurin series.