Integrals Parametric Sphere Vectors 6Ddf3B
1. **Problem:** Determine the convergence or divergence of the integrals:
(a) $$\int_1^{+\infty} \frac{2 + \sin(x^2 + x - 1)}{x - \sqrt{x}} \, dx$$
(b) $$\int_1^{+\infty} \frac{1}{\sqrt{x^{4/3} - e^{-x}}} \, dx$$
**Step 1:** Analyze the behavior of the integrands as $x \to +\infty$.
(a) For large $x$, $x - \sqrt{x} \sim x$ since $\sqrt{x}$ grows slower than $x$.
The numerator $2 + \sin(x^2 + x - 1)$ oscillates between $1$ and $3$.
So the integrand behaves roughly like $\frac{\text{bounded}}{x}$.
Since $\int_1^{+\infty} \frac{1}{x} dx$ diverges (harmonic integral), the integral (a) diverges by comparison.
(b) For large $x$, $e^{-x} \to 0$, so $x^{4/3} - e^{-x} \sim x^{4/3}$.
Thus the integrand behaves like $\frac{1}{\sqrt{x^{4/3}}} = \frac{1}{x^{2/3}}$.
Since $\int_1^{+\infty} x^{-2/3} dx = \int_1^{+\infty} x^{-p} dx$ with $p=2/3 < 1$, this integral diverges.
**Answer:** Both integrals diverge.
2. **Problem:** Parametrized curve $x=2\ln t$, $y=t + \frac{1}{t}$, $t>0$.
(a) Find $y=f(x)$.
**Step 1:** Express $t$ in terms of $x$:
$$x = 2 \ln t \implies \ln t = \frac{x}{2} \implies t = e^{x/2}.$$
**Step 2:** Substitute into $y$:
$$y = e^{x/2} + e^{-x/2} = 2 \cosh\left(\frac{x}{2}\right).$$
So, $$f(x) = 2 \cosh\left(\frac{x}{2}\right).$$
(b) Find tangent line at $t=2$.
**Step 1:** Compute $x(2)$ and $y(2)$:
$$x(2) = 2 \ln 2, \quad y(2) = 2 + \frac{1}{2} = \frac{5}{2}.$$
**Step 2:** Compute derivatives:
$$\frac{dx}{dt} = \frac{2}{t}, \quad \frac{dy}{dt} = 1 - \frac{1}{t^2}.$$
At $t=2$:
$$\frac{dx}{dt} = 1, \quad \frac{dy}{dt} = 1 - \frac{1}{4} = \frac{3}{4}.$$
**Step 3:** Slope of tangent line:
$$\frac{dy}{dx} = \frac{dy/dt}{dx/dt} = \frac{3/4}{1} = \frac{3}{4}.$$
**Step 4:** Equation of tangent line:
$$y - \frac{5}{2} = \frac{3}{4} (x - 2 \ln 2).$$
(c) Find $t$ for horizontal tangent line.
**Step 1:** Horizontal tangent means $\frac{dy}{dx} = 0$.
Since $$\frac{dy}{dx} = \frac{dy/dt}{dx/dt} = \frac{1 - \frac{1}{t^2}}{\frac{2}{t}} = \frac{t^2 - 1}{2t^2}.$$
Set numerator zero:
$$t^2 - 1 = 0 \implies t = 1 \quad (t>0).$$
(d) Compute length from $t=1$ to $t=2$.
**Step 1:** Arc length formula:
$$L = \int_1^2 \sqrt{\left(\frac{dx}{dt}\right)^2 + \left(\frac{dy}{dt}\right)^2} dt.$$
**Step 2:** Compute derivatives:
$$\frac{dx}{dt} = \frac{2}{t}, \quad \frac{dy}{dt} = 1 - \frac{1}{t^2}.$$
**Step 3:** Compute integrand:
$$\sqrt{\left(\frac{2}{t}\right)^2 + \left(1 - \frac{1}{t^2}\right)^2} = \sqrt{\frac{4}{t^2} + 1 - \frac{2}{t^2} + \frac{1}{t^4}} = \sqrt{1 + \frac{2}{t^2} + \frac{1}{t^4}} = \sqrt{\left(1 + \frac{1}{t^2}\right)^2} = 1 + \frac{1}{t^2}.$$
**Step 4:** Integrate:
$$L = \int_1^2 \left(1 + \frac{1}{t^2}\right) dt = \left[t - \frac{1}{t}\right]_1^2 = \left(2 - \frac{1}{2}\right) - (1 - 1) = \frac{3}{2}.$$
(e) Energy of curve portion for $t \in (0,1]$.
**Step 1:** Energy is often proportional to integral of speed squared:
$$E = \int_0^1 \left(\left(\frac{dx}{dt}\right)^2 + \left(\frac{dy}{dt}\right)^2\right) dt = \int_0^1 \left(\frac{4}{t^2} + \left(1 - \frac{1}{t^2}\right)^2\right) dt.$$
**Step 2:** Simplify integrand:
$$\frac{4}{t^2} + 1 - \frac{2}{t^2} + \frac{1}{t^4} = 1 + \frac{2}{t^2} + \frac{1}{t^4}.$$
**Step 3:** Near $t=0$, dominant term is $\frac{1}{t^4}$ which is not integrable:
$$\int_0^1 \frac{1}{t^4} dt$$ diverges.
**Answer:** Energy is infinite.
3. **Problem:** Find center and radius of sphere:
$$x^2 + y^2 + z^2 - 2x + 4z = -3.$$
**Step 1:** Complete the square for $x$ and $z$:
$$x^2 - 2x = (x - 1)^2 - 1,$$
$$z^2 + 4z = (z + 2)^2 - 4.$$
**Step 2:** Rewrite equation:
$$(x - 1)^2 - 1 + y^2 + (z + 2)^2 - 4 = -3,$$
$$(x - 1)^2 + y^2 + (z + 2)^2 = 2.$$
**Step 3:** Center and radius:
Center: $(1, 0, -2)$
Radius: $\sqrt{2}$.
4. **Problem:** Points $A=(1,-1,2)$, $B=(3,-2,3)$, $C=(2,-2,2)$.
(a) Find vectors $\overrightarrow{AB}$ and $\overrightarrow{AC}$.
$$\overrightarrow{AB} = B - A = (3-1, -2+1, 3-2) = (2, -1, 1),$$
$$\overrightarrow{AC} = C - A = (2-1, -2+1, 2-2) = (1, -1, 0).$$
(b) Compute angle $\widehat{BAC}$.
**Step 1:** Use dot product:
$$\overrightarrow{AB} \cdot \overrightarrow{AC} = 2 \cdot 1 + (-1)(-1) + 1 \cdot 0 = 2 + 1 + 0 = 3.$$
**Step 2:** Magnitudes:
$$|\overrightarrow{AB}| = \sqrt{2^2 + (-1)^2 + 1^2} = \sqrt{4 + 1 + 1} = \sqrt{6},$$
$$|\overrightarrow{AC}| = \sqrt{1^2 + (-1)^2 + 0^2} = \sqrt{1 + 1} = \sqrt{2}.$$
**Step 3:** Angle:
$$\cos \theta = \frac{3}{\sqrt{6} \sqrt{2}} = \frac{3}{\sqrt{12}} = \frac{3}{2\sqrt{3}} = \frac{\sqrt{3}}{2}.$$
So,
$$\theta = \frac{\pi}{6} = 30^\circ.$$
(c) Are points aligned?
Check if $\overrightarrow{AB}$ and $\overrightarrow{AC}$ are linearly dependent.
Since $\overrightarrow{AB} = (2,-1,1)$ and $\overrightarrow{AC} = (1,-1,0)$ are not scalar multiples, points are not aligned.
(d) Find plane equation through $A,B,C$.
**Step 1:** Normal vector is cross product:
$$\vec{n} = \overrightarrow{AB} \times \overrightarrow{AC} = \begin{vmatrix} \mathbf{i} & \mathbf{j} & \mathbf{k} \\ 2 & -1 & 1 \\ 1 & -1 & 0 \end{vmatrix} = \mathbf{i}((-1)(0) - 1(-1)) - \mathbf{j}(2(0) - 1(1)) + \mathbf{k}(2(-1) - (-1)(1)) = \mathbf{i}(0 + 1) - \mathbf{j}(0 - 1) + \mathbf{k}(-2 + 1) = (1,1,-1).$$
**Step 2:** Plane equation:
$$1(x - 1) + 1(y + 1) - 1(z - 2) = 0,$$
$$x - 1 + y + 1 - z + 2 = 0,$$
$$x + y - z + 2 = 0.$$