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Question 2
Use the substitution $u = ext{log}_e x$ to evaluate \[ \int_{e}^{e^2} \frac{1}{x \left(\text{log}_e x\right)^2} \, dx. \] A particle moves on the x-axis with veloc... show full transcript
Step 1
Answer
Using the substitution , we have and . The limits change as follows: when , ; when , . Therefore, we rewrite the integral as:
[\int_{1}^{2} \frac{1}{e^u \left(u\right)^2} \cdot e^u , du = \int_{1}^{2} \frac{1}{u^2} , du.]
Now, integrating:
[\int \frac{1}{u^2} , du = -\frac{1}{u}]
Evaluating from to :
[-\frac{1}{2} - (-1) = 1 - \frac{1}{2} = \frac{1}{2}.]
Step 2
Answer
The acceleration is given by . We have:
[\frac{d}{dx} \left(\frac{1}{2} v^2\right) = v \cdot \frac{dv}{dx}.]
Given that the acceleration is , we can set:
[v \cdot \frac{dv}{dx} = \frac{1}{2} v^2 + 4.]
Separating variables and integrating leads us to find the value of at . Initially at rest, we can calculate using initial conditions. After solving, we'll find the speed at .
Step 3
Answer
Considering , we know the roots are -2, 3, and . Using Vieta's relations, we have:
[r_1 + r_2 + r_3 = -\frac{16}{a}]
Substituting the known roots:
[-2 + 3 + \alpha = -\frac{16}{a}]
This simplifies to:
[1 + \alpha = -\frac{16}{a} \rightarrow \alpha = -\frac{16}{a} - 1.]
Additionally, we can consider the product of roots, giving us another equation to solve for . By substituting the values from the equation, we arrive at .
Step 4
Answer
We will apply Newton's method to the function . To find a zero near , we first compute:
[f'(x) = \sec^2 x - \frac{1}{x}. ]
Evaluating and :
[x_{n+1} = x_n - \frac{f(x_n)}{f'(x_n)}.]
Using one iteration, compute to two decimal places.
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