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In the following exercises, suppose y = f ( x ) is defined for all x . For each description, sketch a graph with the indicated property.

Discontinuous at x = 1 with lim x −1 f ( x ) = −1 and lim x 2 f ( x ) = 4

Answers may vary; see the following example:
The graph of a piecewise function with two parts. The first part is an increasing curve that exists for x < 1. It ends at (1,1). The second part is an increasing line that exists for x > 1. It begins at (1,3).

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Discontinuous at x = 2 but continuous elsewhere with lim x 0 f ( x ) = 1 2

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Determine whether each of the given statements is true. Justify your response with an explanation or counterexample.

f ( t ) = 2 e t e t is continuous everywhere.

False. It is continuous over ( , 0 ) ( 0 , ) .

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If the left- and right-hand limits of f ( x ) as x a exist and are equal, then f cannot be discontinuous at x = a .

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If a function is not continuous at a point, then it is not defined at that point.

False. Consider f ( x ) = { x if x 0 4 if x = 0 .

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According to the IVT, cos x sin x x = 2 has a solution over the interval [ −1 , 1 ] .

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If f ( x ) is continuous such that f ( a ) and f ( b ) have opposite signs, then f ( x ) = 0 has exactly one solution in [ a , b ] .

False. Consider f ( x ) = cos ( x ) on [ π , 2 π ] .

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The function f ( x ) = x 2 4 x + 3 x 2 1 is continuous over the interval [ 0 , 3 ] .

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If f ( x ) is continuous everywhere and f ( a ) , f ( b ) > 0 , then there is no root of f ( x ) in the interval [ a , b ] .

False. The IVT does not work in reverse! Consider ( x 1 ) 2 over the interval [ −2 , 2 ] .

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[T] The following problems consider the scalar form of Coulomb’s law, which describes the electrostatic force between two point charges, such as electrons. It is given by the equation F ( r ) = k e | q 1 q 2 | r 2 , where k e is Coulomb’s constant, q i are the magnitudes of the charges of the two particles, and r is the distance between the two particles.

To simplify the calculation of a model with many interacting particles, after some threshold value r = R , we approximate F as zero.

  1. Explain the physical reasoning behind this assumption.
  2. What is the force equation?
  3. Evaluate the force F using both Coulomb’s law and our approximation, assuming two protons with a charge magnitude of 1.6022 × 10 −19 coulombs (C) , and the Coulomb constant k e = 8.988 × 10 9 Nm 2 / C 2 are 1 m apart. Also, assume R < 1 m . How much inaccuracy does our approximation generate? Is our approximation reasonable?
  4. Is there any finite value of R for which this system remains continuous at R ?
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Instead of making the force 0 at R , instead we let the force be 10 −20 for r R . Assume two protons, which have a magnitude of charge 1.6022 × 10 −19 C , and the Coulomb constant k e = 8.988 × 10 9 Nm 2 / C 2 . Is there a value R that can make this system continuous? If so, find it.

R = 0.0001519 m

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Recall the discussion on spacecraft from the chapter opener. The following problems consider a rocket launch from Earth’s surface. The force of gravity on the rocket is given by F ( d ) = m k / d 2 , where m is the mass of the rocket, d is the distance of the rocket from the center of Earth, and k is a constant.

[T] Determine the value and units of k given that the mass of the rocket on Earth is 3 million kg. ( Hint : The distance from the center of Earth to its surface is 6378 km.)

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[T] After a certain distance D has passed, the gravitational effect of Earth becomes quite negligible, so we can approximate the force function by F ( d ) = { m k d 2 if d < D 10,000 if d D . Find the necessary condition D such that the force function remains continuous.

D = 63.78 km

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As the rocket travels away from Earth’s surface, there is a distance D where the rocket sheds some of its mass, since it no longer needs the excess fuel storage. We can write this function as F ( d ) = { m 1 k d 2 if d < D m 2 k d 2 if d D . Is there a D value such that this function is continuous, assuming m 1 m 2 ?

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Prove the following functions are continuous everywhere

f ( θ ) = sin θ

For all values of a , f ( a ) is defined, lim θ a f ( θ ) exists, and lim θ a f ( θ ) = f ( a ) . Therefore, f ( θ ) is continuous everywhere.

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Where is f ( x ) = { 0 if x is irrational 1 if x is rational continuous?

Nowhere

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Practice Key Terms 9

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Source:  OpenStax, Calculus volume 1. OpenStax CNX. Feb 05, 2016 Download for free at http://cnx.org/content/col11964/1.2
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