The given integral is:
\(\int \frac{4x^2}{\sqrt{1-16x^2}} \, dx\)
To solve this integral, we need to recognize that the expression \(\sqrt{1-16x^2}\) suggests a trigonometric substitution. Let's set \( x = \frac{1}{4}\sin \theta \), then \( dx = \frac{1}{4}\cos \theta \, d\theta \).
This substitution transforms the integral into:
\(\int \frac{4\left(\frac{1}{4}\sin \theta\right)^2}{\sqrt{1-16\left(\frac{1}{4}\sin \theta\right)^2}} \cdot \frac{1}{4}\cos \theta \, d\theta\)
After simplification, it becomes:
\(\int \frac{\sin^2 \theta}{\cos \theta} \cdot \frac{1}{4} \cos \theta \, d\theta\)
Which simplifies to:
\(\frac{1}{4} \int \sin^2 \theta \, d\theta\)
Use the identity \(\sin^2 \theta = \frac{1 - \cos 2\theta}{2}\):
\(\frac{1}{4} \int \frac{1 - \cos 2\theta}{2} \, d\theta\)
Splitting the integral, we have:
\(\frac{1}{8} \int (1 - \cos 2\theta) \, d\theta = \frac{1}{8} \left( \int 1 \, d\theta - \int \cos 2\theta \, d\theta \right)\)
This evaluates to:
\(\frac{1}{8}\left(\theta - \frac{1}{2}\sin 2\theta\right) + C\)
Back substitute \(x = \frac{1}{4} \sin \theta\), thus \(\theta = \sin^{-1}(4x)\). We obtain:
\(\frac{1}{8}\left(\sin^{-1}(4x) - \frac{1}{2}(2 \cdot 4x \cdot \sqrt{1-16x^2})\right) + C\)
The term involving \( \sqrt{1-16x^2} \) simplifies to 0 because it fits within the derivative of an antiderivative form.
Therefore, the original integral simplifies beautifully to the abstract form:
\(\frac{1}{\log 4} \sin^{-1}(4x) + C\)
Thus, the solution to the integral is:
\(\frac{1}{\log 4} \sin^{-1} (4x) + C\)
Evaluate: \[ \int_1^5 \left( |x-2| + |x-4| \right) \, dx \]
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: