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Evaluate the following limits. $$\lim _{t \rightarrow 0}\left(\frac{\tan t}{t} \mathbf{i}-\frac{3 t}{\sin t} \mathbf{j}+\sqrt{t+1} \mathbf{k}\right)$$

Short Answer

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Question: Determine if the limit of the three-dimensional vector exists: $$\lim_{t\to 0} \left(\frac{\tan{t}}{t}, \frac{3t}{\sin{t}}, \sqrt{t+1}\right)$$ Answer: The limit does not exist.

Step by step solution

01

Evaluating the first component

The first component is $$\lim _{t \rightarrow 0}\left(\frac{\tan t}{t}\right)$$. We can rewrite this using the sine and cosine functions: $$\lim _{t \rightarrow 0}\left(\frac{\sin t}{t \cos t}\right)$$ Now, applying L'Hopital's rule, we'll differentiate the numerator and the denominator with respect to t: $$= \lim _{t \rightarrow 0}\left(\frac{\cos t}{-\sin t + t \cos t}\right)$$ Now plugging in the value of t = 0: $$= \frac{\cos 0}{-\sin 0 + 0 \cos 0} = \frac{1}{0}$$ Since the limit tends to infinity, the first component does not converge to a finite value, and thus, we cannot find the limit of this vector. If the first component had converged, we would proceed to steps 2 and 3, where we would evaluate limits for the second and third components. However, since the first component did not converge, we can stop here and conclude that the given limit does not exist.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Vector Calculus
Vector calculus is a branch of mathematics focused on vector fields, which is essential when working with multivariable functions and real-world problems in physics and engineering. In this context, vectors are quantities that have both magnitude and direction. In this exercise, the given limit is expressed as a vector with each component representing a different limit to be evaluated individually.
When dealing with limits of vector functions, each component of the vector function needs to be assessed separately. This is important because the convergence or divergence of the vector as a whole depends on all of its components. Therefore, if any component does not converge to a finite value, the entire vector limit does not exist.
  • The method involves simplifying each part of the vector function and applying limit laws.
  • Each component is treated like a scalar function, allowing the use of standard limit properties.
  • To determine the existence of a vector limit, check if each component individually converges to a finite number.
L'Hopital's Rule
L'Hopital's Rule is a powerful tool used in calculus to evaluate limits that initially result in indeterminate forms like \( \frac{0}{0} \) or \( \frac{\infty}{\infty} \). In this exercise, this rule is employed to attempt finding the limit of the first component, \( \lim _{t \rightarrow 0} \left(\frac{\tan t}{t}\right) \).
To apply L'Hopital's Rule, follow these guidelines:
  • Ensure that your limit results in an indeterminate form. If so, differentiate the numerator and the denominator separately with respect to the variable.
  • Re-evaluate the limit using the derivatives obtained. Sometimes, it might be necessary to apply L'Hopital's Rule more than once.
In the given problem, differentiation of the numerator and denominator resulted in another expression \( \frac{\cos t}{-\sin t + t \cos t} \) that, after substitution, led to an undefined result \( \frac{1}{0} \). This implies the component does not converge. Therefore, we conclude that the initial vector limit cannot be determined.
Trigonometric Limits
Trigonometric limits are common in calculus, especially involving small angles. The problem at hand requires evaluating limits with trigonometric functions such as \( \tan t \) and \( \sin t \). Understanding fundamental trigonometric limits helps simplify complex expressions.
Consider the key trigonometric limit \( \lim_{t \to 0} \frac{\sin t}{t} = 1 \), which is useful when analyzing small angle behavior and simplifies many trigonometric limit problems.
To evaluate \( \frac{\tan t}{t} \), rewrite tan in terms of sine and cosine, yielding \( \frac{\sin t}{t \cos t} \). From here:
  • If \( \sin t \approx t \), \( \cos t \approx 1 \) as \( t \to 0 \), which simplifies analysis.
  • Use known limits to fill in components as needed, especially when combined with approaches like L'Hopital's Rule.
Recognizing these fundamental limits is crucial for correctly evaluating complex trigonometric expressions in limits, but as shown, it is equally important to understand when a limit does not exist. These concepts not only help with small trigonometric limits but also play a role in advancing further into calculus topics.

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Most popular questions from this chapter

Three-dimensional motion Consider the motion of the following objects. Assume the \(x\) -axis points east, the \(y\) -axis points north, the positive z-axis is vertical and opposite g. the ground is horizontal, and only the gravitational force acts on the object unless otherwise stated. a. Find the velocity and position vectors, for \(t \geq 0\). b. Make a sketch of the trajectory. c. Determine the time of flight and range of the object. d. Determine the maximum height of the object. A golf ball is hit east down a fairway with an initial velocity of \(\langle 50,0,30\rangle \mathrm{m} / \mathrm{s} .\) A crosswind blowing to the south produces an acceleration of the ball of \(-0.8 \mathrm{m} / \mathrm{s}^{2}\).

Designing a baseball pitch A baseball leaves the hand of a pitcher 6 vertical feet above and 60 horizontal feet from home plate. Assume the coordinate axes are oriented as shown in the figure. Figure cannot copy a. Suppose a pitch is thrown with an initial velocity of (130,0,-3) ft/s (about \(90 \mathrm{mi} / \mathrm{hr}\) ). In the absence of all forces except gravity, how far above the ground is the ball when it crosses home plate and how long does it take the pitch to arrive? b. What vertical velocity component should the pitcher use so that the pitch crosses home plate exactly 3 ft above the ground? c. A simple model to describe the curve of a baseball assumes the spin of the ball produces a constant sideways acceleration (in the \(y\) -direction) of \(c \mathrm{ft} / \mathrm{s}^{2} .\) Suppose a pitcher throws a curve ball with \(c=8 \mathrm{ft} / \mathrm{s}^{2}\) (one fourth the acceleration of gravity). How far does the ball move in the \(y\) -direction by the time it reaches home plate, assuming an initial velocity of \((130,0,-3) \mathrm{ft} / \mathrm{s} ?\) d. In part (c), does the ball curve more in the first half of its trip to the plate or in the second half? How does this fact affect the batter? e. Suppose the pitcher releases the ball from an initial position of \langle 0,-3,6\rangle with initial velocity \(\langle 130,0,-3\rangle .\) What value of the spin parameter \(c\) is needed to put the ball over home plate passing through the point (60,0,3)\(?\)

Consider the curve. $$\mathbf{r}(t)=\langle a \cos t+b \sin t, c \cos t+d \sin t, e \cos t+f \sin t\rangle$$ where \(a, b, c, d, e,\) and \(f\) are real numbers. It can be shown that this curve lies in a plane. Graph the following curve and describe it. $$r(t)=(2 \cos t+2 \sin t) i+(-\cos t+2 \sin t) \mathbf{j}+(\cos t-2 \sin t) \mathbf{k}$$

Equal area property Consider the ellipse \(\mathbf{r}(t)=\langle a \cos t, b \sin t\rangle\) for \(0 \leq t \leq 2 \pi .\) where \(a\) and \(b\) are real numbers. Let \(\theta\) be the angle between the position vector and the \(x\) -axis. a. Show that \(\tan \theta=\frac{b}{a} \tan t\). b. Find \(\theta^{\prime}(t)\). c. Recall that the area bounded by the polar curve \(r=f(\theta)\) on the interval \([0, \theta]\) is \(A(\theta)=\frac{1}{2} \int_{0}^{\theta}(f(u))^{2} d u .\) Letting \(f(\theta(t))=|\mathbf{r}(\theta(t))|,\) show that \(A^{\prime}(t)=\frac{1}{2} a b\). d. Conclude that as an object moves around the ellipse, it sweeps out equal areas in equal times.

Evaluate the following definite integrals. $$\int_{1 / 2}^{1}\left(\frac{3}{1+2 t} \mathbf{i}-\pi \csc ^{2}\left(\frac{\pi}{2} t\right) \mathbf{k}\right) d t$$

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