Problem 76
Question
\(\lim _{x \rightarrow 0}\left(\frac{x-1+\cos x}{x}\right)^{1 / x}=\) (A) \(e^{1 / 2}\) (B) \(e^{-1 / 2}\) (C) \(e^{1 / 4}\) (D) None of these
Step-by-Step Solution
Verified Answer
(B) \(e^{-1/2}\).
1Step 1: Rewrite the Expression
Rewrite the expression in terms of a single limit. Given the function, we need to analyze it in the standard exponential form. To do this, recognize that the expression is of the form \(\lim_{x \to 0} \left(1 + \frac{f(x)}{x}\right)^{1/x}\) where \(f(x) = x - 1 + \cos x\).
2Step 2: Analyze the Term Inside the Limit
We first focus on \(f(x) = x - 1 + \cos x\) and need to approximate it as \(x\) tends to zero. Expand \(\cos x\) using the Taylor series expansion around zero: \(\cos x \approx 1 - \frac{x^2}{2}\). Substitute this in to get: \(f(x) = x - 1 + (1 - \frac{x^2}{2}) = x - \frac{x^2}{2}\).
3Step 3: Simplify the Expression Inside the Exponential
Substitute the expanded \(f(x)\) back into the limit expression: \(\frac{f(x)}{x} = \frac{x - \frac{x^2}{2}}{x} = 1 - \frac{x}{2}\). Therefore, the whole expression becomes: \(\lim_{x \to 0} \left(1 + \frac{1 - \frac{x}{2}}{x}\right)^{1/x}\).
4Step 4: Simplify the Exponential Form
Recognize that the expression is now \(\lim_{x \to 0} \left(1 - \frac{1}{2}\right)^{1/x}\), as \(f(x)/x = 1 - \frac{x}{2}\) leads directly to \(-\frac{1}{2}\) when raised to \(1/x\) as \(x\) approaches zero.
5Step 5: Apply Limit Properties
By recognizing the form \(\lim_{x \to 0} \left(1 + \frac{-1/2}{x}\right)^{1/x}\), apply the known limit \( \lim_{u \to 0} \left(1 + u\right)^{1/u} = e\) which results in the expression becoming \(e^{-1/2}\).
6Step 6: Identify the Correct Answer
The simplified exponential expression is \(e^{-1/2}\). Thus, the correct answer is the option provided in the question, which is (B) \(e^{-1/2}\).
Key Concepts
Taylor SeriesLimit PropertiesExponential FormMathematical Approximation
Taylor Series
The Taylor series is a powerful mathematical tool used to approximate functions. It provides a way to express complex functions as an infinite sum of terms calculated from the values of its derivatives at a single point.
By approximating functions with a polynomial, we can simplify calculations and make complex problems more manageable. This is especially useful near the point where the series is expanded, which is usually zero for simplicity.
By approximating functions with a polynomial, we can simplify calculations and make complex problems more manageable. This is especially useful near the point where the series is expanded, which is usually zero for simplicity.
- The Taylor series for a function \(f(x)\) around zero is given by \(f(x) = f(0) + f'(0)x + \frac{f''(0)x^2}{2!} + \cdots\).
- For this exercise, we use the Taylor series for \(\cos x\), which is \(\cos x \approx 1 - \frac{x^2}{2} + \frac{x^4}{4!} - \cdots\).
Limit Properties
Limits allow mathematicians to understand the behavior of a function as the input approaches a particular point, in this case zero. Understanding limits is crucial to analyzing and simplifying expressions in calculus, especially when dealing with expressions that become indeterminate, like \(\frac{0}{0}\).
Some helpful properties of limits include:
Some helpful properties of limits include:
- \(\lim_{x \to a} [f(x) + g(x)] = \lim_{x \to a} f(x) + \lim_{x \to a} g(x)\)
- \(\lim_{x \to a} [f(x) \cdot g(x)] = \lim_{x \to a} f(x) \cdot \lim_{x \to a} g(x)\)
- If \(f(x)\) is continuous at \(a\), then \(\lim_{x \to a} f(x) = f(a)\)
Exponential Form
Exponential forms arise frequently in limits and series due to their unique properties, especially when dealing with the limit definitions like \(\lim_{x \to 0}\). The exponential form \(\left(1 + \frac{f(x)}{x}\right)^{1/x}\) appears often, and using properties of the exponential function can simplify complex limits in calculus.
In the exponential limit equation:\[\lim_{x \to 0} \left(1 + \frac{f(x)}{x}\right)^{1/x} = e^{L}\]
Here, \(L\) is the value that results from the contribution of \(f(x)\) as \(x\) approaches zero. This form is particularly useful because of the approximation \((1 + u)^{1/u} \to e\) as \(u\) approaches zero. In our concept, this allows us to transform a complex-looking limit into a simple expression: \(e^{-1/2}\).
Use of exponential form in calculus facilitates simplification and analysis, showing how intricate expressions contract to a recognizable format.
In the exponential limit equation:\[\lim_{x \to 0} \left(1 + \frac{f(x)}{x}\right)^{1/x} = e^{L}\]
Here, \(L\) is the value that results from the contribution of \(f(x)\) as \(x\) approaches zero. This form is particularly useful because of the approximation \((1 + u)^{1/u} \to e\) as \(u\) approaches zero. In our concept, this allows us to transform a complex-looking limit into a simple expression: \(e^{-1/2}\).
Use of exponential form in calculus facilitates simplification and analysis, showing how intricate expressions contract to a recognizable format.
Mathematical Approximation
Mathematical approximation is an essential aspect of solving calculus problems, as exact solutions are not always feasible due to the complexity of functions. By approximating expressions, we can gain insights into their behavior in simpler terms.
To solve this particular exercise, we approximated \(\cos x\) using a Taylor series to a few terms, recognizing that the contributions of higher degree terms are negligible for small \(x\). This approximation simplified the expression to \(x - \frac{x^2}{2}\), making the limit calculation cleaner.
To solve this particular exercise, we approximated \(\cos x\) using a Taylor series to a few terms, recognizing that the contributions of higher degree terms are negligible for small \(x\). This approximation simplified the expression to \(x - \frac{x^2}{2}\), making the limit calculation cleaner.
- Approximations allow for a clearer understanding of problem behavior near specific points, such as zero.
- They reduce the complexity of a problem, which is particularly useful in turning indeterminate forms into solvable ones using familiar limits and exponential form properties.
Other exercises in this chapter
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View solution Problem 77
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