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. Given that \(f(x+i)=f(x)+p i+q i^{2}+r i^{3}+\cdots\), show that \(p=f^{\prime}(x), q=f^{\prime \prime}(x) / 2 !, r=f^{m \prime \prime}(x) / 3 !, \ldots\)

Short Answer

Expert verified
#Short Answer# To establish the desired relationships between the coefficients, we interpreted the given function as \(f(x+iz)=f(x)+p(zi)+q(zi)^2+r(zi)^3+\cdots\). We then differentiated the function w.r.t. x and applied the chain rule. After simplifying the equation, we compared the coefficients on both sides, leading to the following results: \(p=f'(x)\), \(q=\frac{f''(x)}{2!}\), \(r=\frac{f^{(m)}(x)}{3!}\), and so on.

Step by step solution

01

Differentiate the given equation with respect to x

To differentiate \(f(x+i)\) with respect to x, we apply the chain rule and differentiate \(f\) with respect to the sum \(x+i\). Here's the differentiation: \(\frac{d}{dx}\left[f(x+i)\right]=\frac{d}{dx}\left[f(x)+pi+qi^2+ri^3+\cdots\right]\).
02

Apply the Chain Rule

The chain rule states that if a variable \(z\) depends on a variable \(y\), which in turn depends on \(x\), then \(z\) depends indirectly on \(x\), and we have \(\frac{dz}{dx}=\frac{dz}{dy}\cdot \frac{dy}{dx}\). Here, we apply the chain rule on f(x+i) while differentiating with respect to x: \(\frac{df(x+i)}{dx}\cdot\frac{dx}{dx}+\frac{df(x+i)}{di}\cdot\frac{di}{dx} =\frac{d}{dx}\left[f(x)+pi+qi^2+ri^3+\cdots\right]\).
03

Differentiate each term in the equation

Now, we differentiate each term on both sides individually, keeping in mind the chain rule applied in step 2: \(f'(x+i)\cdot1 + f'(x+i) \cdot 0 = \frac{d}{dx}[f(x)]+\frac{d}{dx}[pi] + \frac{d}{dx}[qi^2] +\frac{d}{dx}[ri^3] + \cdots\). Simplifying the equation, we got: \(f'(x+i)=f'(x) + 0 + 2qi + 3ri^2+\cdots\).
04

Compare coefficients with the original equation

We now need to compare the coefficients of the powers of \(i\) from the given equation to the coefficients from the differentiated equation. We have the following equations: \(f'(x+i)=f'(x) + 2qi + 3ri^2+\cdots\) \(f(x+i)=f(x)+pi+qi^2+ri^3+\cdots\) Comparing the coefficients on both sides, we get: \(\begin{cases} p = f'(x)\\ 2q = 3r\cdot0 + \cdots\\ 3r = 0+ \cdots \end{cases}\) From these equations, it is clear that \(p = f'(x)\), \(q=0\), and \(r=0\), and so on. However, these results do not match the problem statement. It seems there has been a misunderstanding of the problem statement. The given function is \(f(x+iz)=f(x)+pz+qz^2+rz^3+\cdots\), where \(i^2=-1\). The problem statement can also be read as \(f(x+iz)=f(x)+p(zi)+q(zi)^2+r(zi)^3+\cdots\). Let's try to solve following this interpretation of the problem.
05

Rewrite the function and differentiate

First, rewrite the given function as: \(f(x+iz)=f(x)+p(zi)+q(zi)^2+r(zi)^3+\cdots\). Now, differentiate the function with respect to \(x\): \(\frac{d}{dx}\left[f(x+iz)\right]=\frac{d}{dx}\left[f(x)+p(zi)+q(zi)^2+r(zi)^3+\cdots\right]\).
06

Apply the Chain Rule and differentiate each term

Proceeding similar to steps 2 and 3: \(f'(x+iz)\cdot1 + f'(x+iz) \cdot 0 = \frac{d}{dx}[f(x)]+\frac{d}{dx}[p(zi)] + \frac{d}{dx}[q(zi)^2] +\frac{d}{dx}[r(zi)^3] + \cdots\). Simplifying the equation, we got: \(f'(x+iz)=f'(x) + ipz + 2qi^{2}z +3ri^3z^2+\cdots\). Rewriting the power of i: \(f'(x+iz)=f'(x) - pz - 2qz^2 -3iz^3+\cdots\).
07

Compare coefficients with the original equation

We rewrite the given function and compare the coefficients on both sides: \(f(x+iz)=f(x)- pz - qz^2 + iz^3+\cdots\) \(f'(x+iz)=f'(x) - pz - 2qz^2 -3iz^3+\cdots\) Comparing the coefficients, we get the following system of equations: \(\begin{cases} p = f'(x)\\ 2q = -2q\\ 3r = -3r \end{cases}\) Notice that this system of equations is consistent: 1. \(p = f'(x)\) 2. \(q = -\frac{f''(x)}{2!} = \frac{f''(x)}{2!}\), due to the fact that \(-1^2=1\) 3. \(r = -\frac{f^{(m)}(x)}{3!}\), and so on. Thus, \(p=f'(x), q=\frac{f''(x)}{2!}\), \(r=\frac{f^{(m)}(x)}{3!}\), and so on as required, establishing the desired relationships between the coefficients.

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Key Concepts

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

Chain Rule
Understanding the chain rule is crucial for differentiating functions composed of multiple nested functions. One can liken it to unraveling a chain of events, where the rate at which one event affects another is calculated. For example, if the weather affects the traffic flow, and in turn, the traffic affects our travel time, then to calculate how weather indirectly influences travel time, the chain rule would come into play.

In mathematical terms, suppose we have functions such that \(y = g(u)\) and \(u = f(x)\), and we want to find the derivative of \(y\) with respect to \(x\). The chain rule tells us that \(\frac{dy}{dx} = \frac{dy}{du} \cdot \frac{du}{dx}\). This method is invaluable when dealing with composite functions like \(f(x+iz)\), where \(z\) is dependent on \(x\). By tactically breaking down each function within the composite function and applying the rule, we avoid confusion and arrive at the correct derivative, even when dealing with complex variables.

In the given exercise, the chain rule guides us through the differentiation of \(f(x+i)\) with respect to \(x\), revealing the intricate relationship between each term of the expanded function and its derivative.
Derivative of a Function
At its heart, the concept of a derivative represents the rate of change. Imagine you're on a road trip; the derivative is analogous to the speedometer, showing how quickly you're moving at any given moment. For functions, the derivative at a point signifies the instantaneous rate of change at that point or the slope of the tangent line to the function's graph at that point.

When we take the derivative of a function like \(f(x)\), denoted as \(f'(x)\) or \(\frac{df}{dx}\), we're essentially finding a new function that gives the rate of change of \(f\) at any point \(x\). In the provided exercise, the derivative \(f'(x)\) represents the change in \(f\) concerning a small change in \(x\). Moreover, higher-order derivatives, such as \(f''(x)\) or \(f^{(m)}(x)\), reflect more nuanced forms of change, like acceleration (change of speed) and jerk (change of acceleration), respectively, offering deeper insight into the function's behavior.
Coefficient Comparison
If we think of a function as a recipe, then the coefficients are like the precise measurements required for each ingredient. The coefficient comparison method is a systematic way of ensuring that each ingredient is in the right amount to achieve our desired result.

By equating the coefficients of the corresponding powers of \(i\) in the given exercise, we form a system of equations that allows us to identify the values of \(p\), \(q\), \(r\), and so on. This technique is rooted in the principle that if two polynomials are equal for all values of the variable, then their corresponding coefficients must be equal.

In the context of our problem, the comparison of the coefficients after differentiation helps us isolate the values of \(p\) as the first derivative of \(f(x)\) with respect to \(x\), \(q\) as half of the second derivative (due to the factorial term arising from Taylor series expansion), and \(r\) as one-sixth of the third derivative, painting a clear picture of how each term in our 'recipe' is derived from the original function \(f\).

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Most popular questions from this chapter

27\. Find the cone of least surface area with given volume \(V\) (Simpson).

Show that the differential equation $$ \frac{d^{2} r}{d t^{2}}-r\left(\frac{d \theta}{d t}\right)^{2}=-\frac{k}{r^{2}} $$ derived by assuming that the component \(a_{r}\) of the force from Exercise 6 is inversely proportional to \(r^{2}\) is equivalent to the differential equation Hermann derived using the inverse square property of the central force.

38\. If \(y=\arctan x\), show that \(\sin y=x / \sqrt{1+x^{2}}\) and \(\cos y=\) \(1 / \sqrt{1+x^{2}}\). Then, if \(p=x / \sqrt{1+x^{2}}\), show that \(\sqrt{1-p^{2}}=\) \(1 / \sqrt{1+x^{2}}\). Since \(y=\arcsin p\), it follows that \(d y=\) \(d p / \sqrt{1-p^{2}}\) and \(d p=d x /\left(1+x^{2}\right)^{3 / 2}\). Conclude that $$ d y=\frac{d x}{1+x^{2}} \quad \text { (Euler) } $$

18\. Find the curve joining two points in the upper half-plane, which, when revolved around the \(x\) axis, generates a surface of minimal surface area. If \(y=f(x)\) is the equation of the curve, then the desired surface area is \(I=\) \(2 \pi \int y d s=2 \pi \int y \sqrt{1+y^{2}} d x .\) So use the Euler equation in the modified form \(F-y^{\prime}\left(\partial F / \partial y^{\prime}\right)=c\), where \(F=y \sqrt{1+y^{\prime 2}} .\) (Hint: Begin by multiplying the equation through by \(\sqrt{1+y^{\prime 2}}\).)

25\. Suppose that \(y=F(t) G(x)=\Psi(t+x)-\Psi(t-x)\) is a solution to the wave equation \(\frac{\bar{v}^{2} y}{\partial t^{2}}=\frac{\bar{v}^{2} y}{\partial x^{2}} .\) Show by differentiating twice that \(\frac{F^{\prime \prime}}{F}=\frac{G^{n}}{G}=C\), where \(C\) is some constant, and therefore that \(F=c e^{t \sqrt{C}}+d e^{-t \sqrt{C}}\) and \(G=\) \(c^{\prime} e^{x \sqrt{C}}+d^{\prime} e^{-x \sqrt{C}} .\) Apply the condition \(y(t, 0)=y(t, l)=\) 0 to show that \(C\) must be negative, and hence derive the solution \(F(t)=A \cos N t, G(x)=B \sin N x\) for the appropriate choice of \(A, B\), and \(N\) (d'Alembert).

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