Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

Sketch the graph of the given function. In each case determine whether \(f\) is continuous, piecewise continuous, or neither on the interval \(0 \leq t \leq 3 .\) $$ f(t)=\left\\{\begin{array}{ll}{t^{2},} & {0 \leq t \leq 1} \\ {2+t,} & {1

Short Answer

Expert verified
Given a function defined by: - \(f(t) = t^2\) for \(0 \leq t \leq 1\) - \(f(t) = 2+t\) for \(1 < t \leq 2\) - \(f(t) = 6-t\) for \(2 < t \leq 3\) After analyzing and sketching the function, we found that the function is discontinuous at \(t=1\) but continuous at \(t=2\). Therefore, the function is considered piecewise continuous on the interval \(0 \leq t \leq 3\).

Step by step solution

01

Sketch the graph of each piece of the function

We need to sketch the graph of the function in each of the given intervals: \(t^2\) for \(0 \leq t \leq 1\), \(2+t\) for \(1<t\leq 2\), and \(6-t\) for \(2<t\leq 3\).
02

Determine continuity at transition points

Now, we need to check the continuousness of the function at the transition points between the intervals. There are two points to check - \(t=1\) and \(t=2\). For \(t=1\), we have: - From the first interval: \(f(t) = t^2 \Rightarrow f(1) = 1^2 = 1\) - From the second interval: \(f(t) = 2 + t \Rightarrow f(1) = 2 + 1 = 3\) The function is discontinuous at \(t=1\) because the limits from the left and right do not match (\(1 \neq 3\)). For \(t=2\), we have: - From the second interval: \(f(t) = 2 + t \Rightarrow f(2) = 2 + 2 = 4\) - From the third interval: \(f(t) = 6 - t \Rightarrow f(2) = 6 - 2 = 4\) The function is continuous at \(t=2\) because the limits from the left and right match (\(4 = 4\)).
03

Determine the classification of the function on the interval \(0 \leq t \leq 3\)

Since the function is discontinuous at \(t=1\), it is not continuous on the interval \(0 \leq t \leq 3\). However, the function has only one point of discontinuity, so it is piecewise continuous on the interval \(0 \leq t \leq 3\).

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Find the inverse Laplace transform of the given function. $$ F(s)=\frac{2(s-1) e^{-2 s}}{s^{2}-2 s+2} $$

The Tautochrone. A problem of interest in the history of mathematics is that of finding the tautochrone-the curve down which a particle will slide freely under gravity alone, reaching the bottom in the same time regardless of its starting point on the curve. This problem arose in the construction of a clock pendulum whose period is independent of the amplitude of its motion. The tautochrone was found by Christian Huygens \((1629-\) \(1695)\) in 1673 by geometrical methods, and later by Leibniz and Jakob Bernoulli using analytical arguments. Bernoulli's solution (in \(1690)\) was one of the first occasions on which a differential equation was explicitly solved. The Tautochrone. A problem of interest in the history of mathematics is that of finding the tautochrone-the curve down which a particle will slide freely under gravity alone, reaching the bottom in the same time regardless of its starting point on the curve. This problem arose in the construction of a clock pendulum whose period is independent of the amplitude of its motion. The tautochrone was found by Christian Huygens \((1629-\) \(1695)\) in 1673 by geometrical methods, and later by Leibniz and Jakob Bernoulli using analytical arguments. Bernoulli's solution (in \(1690)\) was one of the first occasions on which a differential equation was explicitly solved. The geometrical configuration is shown in Figure \(6.6 .2 .\) The starting point \(P(a, b)\) is joined to the terminal point \((0,0)\) by the arc \(C .\) Arc length \(s\) is measured from the origin, and \(f(y)\) denotes the rate of change of \(s\) with respect to \(y:\) $$ f(y)=\frac{d s}{d y}=\left[1+\left(\frac{d x}{d y}\right)^{2}\right]^{1 / 2} $$ Then it follows from the principle of conservation of energy that the time \(T(b)\) required for a particle to slide from \(P\) to the origin is $$ T(b)=\frac{1}{\sqrt{2 g}} \int_{0}^{b} \frac{f(y)}{\sqrt{b-y}} d y $$

Recall that \(\cosh b t=\left(e^{b t}+e^{-b t}\right) / 2\) and \(\sinh b t=\left(e^{b t}-e^{-b t}\right) / 2 .\) In each of Problems 7 through 10 find the Laplace transform of the given function; \(a\) and \(b\) are real constants. $$ e^{a t} \cosh b t $$

Using integration by parts, find the Laplace transform of the given function; \(n\) is a positive integer and \(a\) is a real constant. $$ t e^{a t} $$

Suppose that \(f\) and \(f^{\prime}\) are continuous for \(t \geq 0\), and of exponential order as \(t \rightarrow \infty .\) Show by integration by parts that if \(F(s)=\mathcal{L}(f(t))\), then \(\lim _{s \rightarrow \infty} F(s)=0\). The result is actually true under less restrictive conditions, such as those of Theorem \(6.1 .2 .\)

See all solutions

Recommended explanations on Math Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free