Integration by parts, a powerful technique in calculus, provides the key to unlocking the mysteries surrounding the antiderivative of ln(x). Specifically, exploring functions requires a solid understanding of mathematical software like Mathematica for verifying solutions and performing complex calculations. The concept of natural logarithm, denoted as ln(x), plays a fundamental role, and the rules defined by Gottfried Wilhelm Leibniz, a notable mathematician and logician, are essential when exploring its antiderivative.
Unveiling the Mystery: The Antiderivative of ln(x) Explained!
This article aims to comprehensively explain how to find the antiderivative of the natural logarithm function, ln(x). We will break down the process step-by-step, providing clear explanations and examples. The core focus will remain on understanding and applying the technique to solve for the antiderivative of ln(x).
Understanding the Basics: ln(x) and Antiderivatives
Before diving into the calculation, let’s ensure a solid foundation. We’ll review what ln(x) represents and what taking an antiderivative means.
What is ln(x)?
- ln(x) represents the natural logarithm of x.
- It answers the question: "To what power must the number e (Euler’s number, approximately 2.71828) be raised to equal x?".
- The domain of ln(x) is all positive real numbers (x > 0).
- Understanding the graph of ln(x) is helpful. It starts at negative infinity as x approaches 0, passes through the point (1,0), and increases slowly as x increases.
What is an Antiderivative?
- An antiderivative of a function f(x) is a function F(x) whose derivative is f(x). Mathematically, F'(x) = f(x).
- Finding an antiderivative is also known as integration.
- Antiderivatives are not unique. We add a constant of integration, usually denoted by "C", because the derivative of a constant is always zero. Therefore, if F(x) is an antiderivative of f(x), then F(x) + C is also an antiderivative.
- The antiderivative of f(x) is represented as ∫f(x) dx.
Finding the Antiderivative of ln(x): Integration by Parts
The standard method for finding the antiderivative of ln(x) is integration by parts.
The Integration by Parts Formula
Integration by parts is based on the product rule for differentiation. It states:
∫u dv = uv – ∫v du
Where:
- u and v are functions of x.
- du is the derivative of u.
- dv is the derivative of v.
The trick is choosing the appropriate u and dv.
Applying Integration by Parts to ln(x)
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Choosing u and dv:
- Let u = ln(x)
- Let dv = dx
The reasoning behind this choice is that the derivative of ln(x) is a simple expression (1/x), which will simplify the subsequent integration.
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Finding du and v:
- du = (1/x) dx (Derivative of ln(x))
- v = x (Antiderivative of dx, i.e., ∫dx = x)
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Applying the Formula:
∫ln(x) dx = (ln(x))(x) – ∫x (1/x) dx
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Simplifying:
∫ln(x) dx = x ln(x) – ∫1 dx
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Integrating ∫1 dx:
∫1 dx = x
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The Final Result:
∫ln(x) dx = x ln(x) – x + C
Therefore, the antiderivative of ln(x) is x ln(x) – x + C.
Verification: Differentiating the Result
To verify that we have correctly found the antiderivative, we can differentiate our result:
d/dx [x ln(x) – x + C]
Applying the product rule to x ln(x):
d/dx [x ln(x)] = (1)(ln(x)) + x(1/x) = ln(x) + 1
Differentiating the rest of the expression:
d/dx [-x + C] = -1 + 0 = -1
Combining these results:
ln(x) + 1 – 1 = ln(x)
Since the derivative of x ln(x) – x + C is ln(x), our antiderivative is correct.
Examples of Applying the Antiderivative of ln(x)
Here are a couple of examples demonstrating how to use the antiderivative of ln(x).
Example 1: Definite Integral
Evaluate the definite integral: ∫1e ln(x) dx
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We already know that the antiderivative of ln(x) is x ln(x) – x + C. We can drop the constant C when working with definite integrals.
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Apply the Fundamental Theorem of Calculus:
∫1e ln(x) dx = [e ln(e) – e] – [1 ln(1) – 1]
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Simplify:
- ln(e) = 1
- ln(1) = 0
Therefore:
∫1e ln(x) dx = [e(1) – e] – [1(0) – 1] = [e – e] – [0 – 1] = 0 – (-1) = 1
Example 2: Indefinite Integral with a Constant Multiple
Find the antiderivative of 3 ln(x).
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Use the constant multiple rule: ∫kf(x) dx = k∫f(x) dx, where k is a constant.
∫3 ln(x) dx = 3 ∫ln(x) dx
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We know ∫ln(x) dx = x ln(x) – x + C
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Substitute:
3 ∫ln(x) dx = 3 [x ln(x) – x + C]
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Distribute and simplify (remembering that 3C is still a constant, which we can represent as C):
3x ln(x) – 3x + 3C = 3x ln(x) – 3x + C
Therefore, the antiderivative of 3 ln(x) is 3x ln(x) – 3x + C.
FAQs: Decoding the Antiderivative of ln(x)
Have lingering questions about finding the antiderivative of ln(x)? Here are some common ones to help you solidify your understanding.
What exactly is the antiderivative of ln(x)?
The antiderivative of ln(x) is xln(x) – x + C, where C is the constant of integration. Remember, taking the derivative of xln(x) – x will result in ln(x).
Why isn’t the antiderivative of ln(x) simply 1/x?
1/x is actually the derivative of ln(x), not the antiderivative. Finding the antiderivative involves working backward from the derivative, and in this case, the process requires integration by parts to arrive at x*ln(x) – x + C.
How is integration by parts used to find the antiderivative of ln(x)?
We treat ln(x) as u and 1 as dv in the integration by parts formula (∫u dv = uv – ∫v du). This leads to splitting ln(x) into components that are easier to integrate, ultimately revealing its antiderivative.
Can I check if I found the correct antiderivative of ln(x)?
Absolutely! The best way to verify is to take the derivative of your result. If the derivative equals ln(x), you’ve correctly found the antiderivative of ln(x). Don’t forget to include the "+ C" because the derivative of any constant is zero.
So there you have it! Mastering the antiderivative of ln(x) might seem tricky at first, but with a little practice, you’ll be solving these integrals like a pro. Now go forth and conquer those calculus problems!