\(\frac{9}{2}\)
\(\frac{9}{log_e{10}}\)
\(\frac{9}{2}\)\(log_e10\)
To solve the given integral problem, we need to find the sum of \( f(e^3) \) and \( f(e^{-3}) \), where \( f(\alpha) = \int_{1}^{\alpha} \frac{\log_{10} t}{1+t} \, dt \).
First, observe the function \( f(\alpha) \):
Using substitution on \( f(\alpha) \), we have:
\[ \begin{align*} f(\alpha) &= \int_{1}^{\alpha} \frac{\log_{10} t}{1+t} \, dt = \int_{1}^{\alpha} \frac{\log_{10} t}{1+t} \, dt \\ & = \int_{1}^{1/\alpha} \frac{\log_{10} \left(\frac{1}{x}\right)}{1+\frac{1}{x}} \left(-\frac{1}{x^2}\right) dx \\ & = -\int_{1}^{1/\alpha} \frac{-\log_{10} x}{x+1} \, dx \\ & = \int_{1}^{1/\alpha} \frac{\log_{10} x}{1+x} \, dx. \end{align*} \]
We note that \( f(\alpha) = -f\left(\frac{1}{\alpha}\right) \) due to symmetry and the properties of logarithms. Therefore,
\[ f(e^3) + f(e^{-3}) = \left(\int_{1}^{e^3} \frac{\log_{10} t}{1+t} \, dt \right) + \left(\int_{1}^{e^{-3}} \frac{\log_{10} t}{1+t} \, dt \right) \]
Combine the integrals, changing limits back from 1 to \( e^3 \) and \( e^{-3} \). By symmetry, the sum is simplified to:
\[ f(e^3) + f(e^{-3}) = 2 \times \int_{1}^{e^3} \frac{\log_{10} t}{1+t} \, dt \approx \frac{9}{2} \log_{e} 10 \]
Given the options, the correct answer is:
\(\frac{9}{2}\)\( \log_e 10 \)
The heat generated in 1 minute between points A and B in the given circuit, when a battery of 9 V with internal resistance of 1 \(\Omega\) is connected across these points is ______ J. 
The representation of the area of a region under a curve is called to be as integral. The actual value of an integral can be acquired (approximately) by drawing rectangles.
Also, F(x) is known to be a Newton-Leibnitz integral or antiderivative or primitive of a function f(x) on an interval I.
F'(x) = f(x)
For every value of x = I.
Integral calculus helps to resolve two major types of problems: