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Find the values of the derivatives. $$\left.\frac{d y}{d x}\right|_{x=\sqrt{3}} \text { if } y=1-\frac{1}{x}$$

Short Answer

Expert verified
The derivative at \( x = \sqrt{3} \) is \( \frac{1}{3} \).

Step by step solution

01

Understanding the Problem

We are given a function \( y = 1 - \frac{1}{x} \) and need to find its derivative at \( x = \sqrt{3} \). This entails computing the derivative and then evaluating it at the specified point.
02

Differentiating the Function

The function \( y = 1 - \frac{1}{x} \) can be differentiated using basic calculus rules. Differentiation of \( 1 \) is \( 0 \), and using the power rule, the derivative of \( -\frac{1}{x} \) is \( \frac{1}{x^2} \). Thus, \( \frac{d y}{d x} = \frac{1}{x^2} \).
03

Evaluating the Derivative at x = √3

Substitute \( x = \sqrt{3} \) into the derivative \( \frac{d y}{d x} = \frac{1}{x^2} \). This gives \( \frac{1}{(\sqrt{3})^2} = \frac{1}{3} \).
04

Conclusion

The derivative of the function \( y = 1 - \frac{1}{x} \) at \( x = \sqrt{3} \) is \( \frac{1}{3} \).

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Key Concepts

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

Differentiation
Differentiation is the process of finding the derivative of a function. A derivative represents the rate at which a function is changing at any given point. It helps us understand how variables are linked and how they influence each other over a tiny interval. In simple terms, differentiation is like measuring how steep a hill is at a particular spot. When we differentiate a function, we are looking at how the value of the function changes as the input changes slightly.
To differentiate a function like the one in our problem, we apply specific rules of calculus, which is a branch of mathematics centered around change. This gives us a new function, called the derivative, that tells us the slope of the tangent line to the curve at any point.
Understanding differentiation allows us to solve many real-world problems, from physics and engineering to economics and biology, by predicting how a system will behave when small changes occur.
Power Rule
The power rule is a fundamental technique in calculus used to differentiate functions of the form \(x^n\), where \(n\) is any real number. It states that if \(y = x^n\), its derivative \(\frac{dy}{dx}\) is given by \(nx^{n-1}\). This rule simplifies the differentiation process significantly and is applicable to both positive and negative powers, as well as fractional exponents.
In our original exercise, the function involves the term \(-\frac{1}{x}\), which can be rewritten using exponents as \(-x^{-1}\). By applying the power rule, \(n = -1\), we find the derivative of this term to be \(x^{-2}\) or \(\frac{1}{x^2}\), because \(-1 \times x^{-2} = x^{-2}\). This showcases the utility of the power rule in tackling problems involving different types of exponents smoothly.
This powerful tool helps to quickly evaluate how functions behave and changes are involved, without the need for complex algebraic manipulations.
Evaluating Derivatives
Once a derivative is determined, evaluating it at a specific point gives a tangible value that conveys how the function is changing exactly at that point. In our problem, after differentiating the function, we evaluated it at \(x = \sqrt{3}\). This step involves substituting \(x = \sqrt{3}\) into the derived expression \(\frac{1}{x^2}\) to find the rate of change at that specific location.
In practice, evaluating a derivative provides insights such as velocity of an object, gradient of a surface, or rate of profit growth. It converts the general formula obtained from differentiation into a specific, usable number.
For our function, by substituting \(x = \sqrt{3}\), we calculated \(\frac{1}{3}\), which shows that at \(x = \sqrt{3}\), the function is slowly increasing. This precise rate of change can be critical in applications such as predicting future values or making decisions based on instant slopes.

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Most popular questions from this chapter

Measuring acceleration of gravity When the length \(L\) of a clock pendulum is held constant by controlling its temperature, the pendulum's period \(T\) depends on the acceleration of gravity g. The period will therefore vary slightly as the clock is moved from place to place on the earth's surface, depending on the change in g. By keeping track of \(\Delta T,\) we can estimate the variation in \(g\) from the equation \(T=2 \pi(L / g)^{1 / 2}\) that relates \(T, g,\) and \(L .\) $$ \begin{array}{l}{\text { a. With } L \text { held constant and } g \text { as the independent variable, }} \\ {\text { calculate } d T \text { and use it to answer parts (b) and (c). }} \\ {\text { b. If } g \text { increases, will } T \text { increase or decrease? Will a pendulum }} \\ {\text { clock speed up or slow down? Explain. }}\end{array} $$ $$ \begin{array}{l}{\text { c. A clock with a } 100 \text { -cm pendulum is moved from a location }} \\ {\text { where } g=980 \mathrm{cm} / \mathrm{sec}^{2} \text { to a new location. This increases the }} \\ {\text { period by } d T=0.001 \mathrm{sec} . \text { Find } d g \text { and estimate the value of }} \\\ {g \text { at the new location. }}\end{array} $$

In Exercises \(35-40,\) write a differential formula that estimates the given change in volume or surface area. $$ \begin{array}{l}{\text { The change in the lateral surface area } S=2 \pi r h \text { of a right circu- }} \\ {\text { lar cylinder when the height changes from } h_{0} \text { to } h_{0}+d h \text { and the }} \\ {\text { radius does not change }}\end{array} $$

Find both \(d y / d x\) (treating \(y\) as a differentiable function of \(x\) ) and \(d x / d y\) (treating \(x\) as a differentiable function of \(y )\) . How do \(d y / d x\) and \(d x / d y\) seem to be related? Explain the relationship geometrically in terms of the graphs. \begin{equation} x y^{3}+x^{2} y=6 \end{equation}

If \(x^{2} y^{3}=4 / 27\) and \(d y / d t=1 / 2,\) then what is \(d x / d t\) when \(x=2 ?\)

The linearization is the best linear approximation Suppose that \(y=f(x)\) is differentiable at \(x=a\) and that \(g(x)=\) \(m(x-a)+c\) is a linear function in which \(m\) and \(c\) are constants. If the error \(E(x)=f(x)-g(x)\) were small enough near \(x=a\) we might think of using \(g\) as a linear approximation of \(f\) instead of the linearization \(L(x)=f(a)+f^{\prime}(a)(x-a) .\) Show that if we impose on \(g\) the conditions $$ \begin{array}{l}{\text { 1. } E(a)=0} \\ {\text { 2. } \lim _{x \rightarrow a} \frac{E(x)}{x-a}=0}\end{array} $$ then \(g(x)=f(a)+f^{\prime}(a)(x-a) .\) Thus, the linearization \(L(x)\) gives the only linear approximation whose error is both zero at \(x=a\) and negligible in comparison with \(x-a\) .

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