Mathematics

Linear Approximations and Differentials

Linear approximations and differentials are mathematical tools used to estimate the value of a function near a specific point. The linear approximation is a straight-line approximation to a function, while the differential represents the change in the function's value due to a small change in the independent variable. These concepts are particularly useful in calculus for making quick and accurate estimations.

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8 Key excerpts on "Linear Approximations and Differentials"

  • Book cover image for: Calculus
    eBook - PDF

    Calculus

    Single Variable

    • Carl V. Lutzer, H. T. Goodwill(Authors)
    • 2011(Publication Date)
    • Wiley
      (Publisher)
    Section 4.1 Linear Approximation 246 z Common Difficulties with Differentials Some students mistake dh for h 0 , but they are different things. Whereas h 0 tells us the instantaneous rate of change, the differential is a linear approximation of how much change happens. In the story of the model rocket, for example, the derivative is h 0 and has units of ft/sec, while the differential dh has units of feet. Units can help you reason your way to or through a formula. You should know • the terms linear approximation, linearization, Newton’s method, converge, diverge, and differential; • that Newton’s method is an algorithm for finding roots of functions; • why Newton’s method “fails” when h 0 (t) = 0; • that differentials give us a linear approximation of change; • that, graphically speaking, the differentials dy tells us about change along the tangent line, whereas Δy is the actual change in the function value. You should be able to • write the linear approximation of f (t) about t 0 ; • execute several steps of Newton’s method by hand; • use a linear approximation of f about t 0 to estimate f (t 0 + Δt); • write the Product Rule and Quotient Rule in terms of differentials; • use differentials to estimate error. z 4.1 Skill Exercises 1. Suppose f (2) = 3 and f 0 (2) = 7. Estimate f (2.001). 2. Suppose f (5) = 12 and f 0 (5) = 3. Estimate f (4.99). 3. Suppose f 0 (8) = 11. Approximate the change in f (t) when t is increased from 8 to 8.0001. 4. Suppose f 0 (-2) = 6. Approximate the change in f (t) when t is decreased from -2 to -2.17. Use linear approximation at t = 1 to estimate the numbers in #5–8. 5. f (1.01) when f (t) = 1 + t 9 6. f (0.9) when f (t) = 13t 8 7. f (0.9) when f (t) = ln(t) 8. f (1.1) when f (t) = sin(πt/6) In #9–12 use linearization at the specified t 0 to approximate the following numbers. 9. √ 24, t 0 = 25 10. 3 √ 65, t 0 = 64 11. cos(3), t 0 = π 12. e 0.1 , t 0 = 0
  • Book cover image for: Calculus
    eBook - PDF

    Calculus

    Early Transcendentals

    • Howard Anton, Irl C. Bivens, Stephen Davis(Authors)
    • 2016(Publication Date)
    • Wiley
      (Publisher)
    3.5 Local Linear Approximation; Differentials 155 DIFFERENTIALS Up to now we have interpreted dy /dx as a single entity representing the derivative of y with respect to x; the symbols “dy” and “dx,” which are called differentials, have had no mean- ings attached to them. Our next goal is to define these symbols in such a way that dy /dx can be treated as an actual ratio. To do this, assume that f is differentiable at a point x, define dx to be an independent variable that can have any real value, and define dy by the formula dy = f  (x) dx (5) If dx = 0, then we can divide both sides of (5) by dx to obtain dy dx = f  (x) (6) This achieves our goal of defining dy and dx so their ratio is f  (x). Formula (5) is said to express (6) in differential form. To interpret (5) geometrically, note that f  (x) is the slope of the tangent line to the graph of f at x. The differentials dy and dx can be viewed as a corresponding rise and run of Figure 3.5.5 this tangent line (Figure 3.5.5). Example 3 Express the derivative with respect to x of y = x 2 in differential form, and discuss the relationship between dy and dx at x = 1. Solution. The derivative of y with respect to x is dy /dx = 2x, which can be expressed in differential form as dy = 2x dx When x = 1 this becomes dy = 2 dx This tells us that if we travel along the tangent line to the curve y = x 2 at x = 1, then a change of dx units in x produces a change of 2 dx units in y. Thus, for example, a run of Figure 3.5.6 dx = 2 units produces a rise of dy = 4 units along the tangent line (Figure 3.5.6). It is important to understand the distinction between the increment Δy and the differen- tial dy. To see the difference, let us assign the independent variables dx and Δx the same value, so dx = Δx.
  • Book cover image for: Calculus
    eBook - PDF

    Calculus

    Multivariable

    • Howard Anton, Irl C. Bivens, Stephen Davis(Authors)
    • 2021(Publication Date)
    • Wiley
      (Publisher)
    Local Linear Approximations We now show that if a function f is differentiable at a point, then it can be very closely approxi- mated by a linear function near that point. For example, suppose that f (x, y) is differentiable at the point (x 0 , y 0 ). Then approximation (3) can be written in the form f (x 0 + Δx, y 0 + Δy) ≈ f (x 0 , y 0 ) + f x (x 0 , y 0 )Δx + f y (x 0 , y 0 )Δy If we let x = x 0 + Δx and y = x 0 + Δy, this approximation becomes Show that if f (x, y) is a linear function, then (14) becomes an equality. f (x, y) ≈ f (x 0 , y 0 ) + f x (x 0 , y 0 )(x − x 0 ) + f y (x 0 , y 0 )(y − y 0 ) (14) which yields a linear approximation of f (x, y). Since the error in this approximation is equal to the error in approximation (3), we conclude that for (x, y) close to (x 0 , y 0 ), the error in (14) will be much smaller than the distance between these two points. When f (x, y) is differ- entiable at (x 0 , y 0 ) we let L(x, y) = f (x 0 , y 0 ) + f x (x 0 , y 0 )(x − x 0 ) + f y (x 0 , y 0 )(y − y 0 ) (15) and refer to L(x, y) as the local linear approximation to f at (x 0 , y 0 ). Explain why the error in approximation (14) is the same as the error in approx- imation (3). Example 4 Let L(x, y) denote the local linear approximation to f (x, y) =  x 2 + y 2 at the point (3, 4). Compare the error in approximating f (3.04, 3.98) =  (3.04) 2 + (3.98) 2 by L(3.04, 3.98) with the distance between the points (3, 4) and (3.04, 3.98). Solution We have f x (x, y) = x  x 2 + y 2 and f y (x, y) = y  x 2 + y 2 818 CHAPTER 13 Partial Derivatives with f x (3, 4) = 3 5 and f y (3, 4) = 4 5 . Therefore, the local linear approximation to f at (3, 4) is given by L(x, y) = 5 + 3 5 (x − 3) + 4 5 (y − 4) Consequently, f (3.04, 3.98) ≈ L(3.04, 3.98) = 5 + 3 5 (0.04) + 4 5 (−0.02) = 5.008 Since f (3.04, 3.98) =  (3.04) 2 + (3.98) 2 ≈ 5.00819 the error in the approximation is about 5.00819 − 5.008 = 0.00019.
  • Book cover image for: Calculus, Metric Edition
    • James Stewart, Daniel K. Clegg, Saleem Watson, , James Stewart, James Stewart, Daniel K. Clegg, Saleem Watson(Authors)
    • 2020(Publication Date)
    Cengage Learning reserves the right to remove additional content at any time if subsequent rights restrictions require it. SECTION 14.4 Tangent Planes and Linear Approximations 1017 ■ Differentials For a differentiable function of one variable, y - f s xd, we define the differential dx to be an independent variable; that is, dx can be given the value of any real number. The dif- ferential of y is then defined as 9 dy - f 9 s xd dx (See Section 2.9.) Figure 6 shows the relationship between the increment Dy and the differential dy : Dy represents the change in height of the curve y - f s xd and dy repre- sents the change in height of the tangent line when x changes by an amount dx - Dx. For a differentiable function of two variables, z - f s x, yd, we define the differentials dx and dy to be independent variables; that is, they can be given any values. Then the differential dz, also called the total differential, is defined by 10 dz - f x s x, yd dx 1 f y s x, yd dy - -z -x dx 1 -z -y dy (Compare with Equation 9.) Sometimes the notation df is used in place of dz. If we take dx - Dx - x 2 a and dy - Dy - y 2 b in Equation 10, then the differen- tial of z is dz - f x sa, bds x 2 ad 1 f y sa, bds y 2 bd So, in the notation of differentials, the linear approximation (4) can be written as f s x, yd < f sa, bd 1 dz Figure 7 is the three-dimensional counterpart of Figure 6 and shows the geometric inter- pretation of the differential dz and the increment Dz: dz represents the change in height of the tangent plane, whereas Dz represents the change in height of the surface z - f s x, yd when s x, yd changes from sa, bd to sa 1 Dx, b 1 Dyd. y x z Îx=dx 0 {a, b, f(a, b)} (a, b, 0) (a+Îx, b+Îy, 0) {a+Îx, b+Îy, f(a+Îx, b+Îy)} f(a, b) f(a, b) Îy=dy tangent plane z-f(a, b)=f x (a, b)(x-a)+f y (a, b)( y-b) surface z=f(x, y) dz Îz EXAMPLE 4 (a) If z - f s x, yd - x 2 1 3xy 2 y 2 , find the differential dz.
  • Book cover image for: Anton's Calculus
    eBook - PDF

    Anton's Calculus

    Early Transcendentals

    • Howard Anton, Irl C. Bivens, Stephen Davis(Authors)
    • 2018(Publication Date)
    • Wiley
      (Publisher)
    Explain your answer. 47. A differential dy is defined to be a very small change in y. 48. The error in approximation (2) is the same as the error in approximation (7). 49. A local linear approximation to a function can never be identically equal to the function. 50. A local linear approximation to a nonconstant function can never be constant. 51–54 Use the differential dy to approximate Δy when x changes as indicated. 51. y = √ 5x − 1; from x = 2 to x = 2.03 52. y = √ x 3 + 8; from x = 1 to x = 0.97 53. y = 1 x 2 + 1 ; from x = 2 to x = 1.96 54. y = x √ 7x + 4; from x = 3 to x = 3.05 55. The side of a square is measured to be 10 ft, with a possible error of ±0.1 ft. (a) Use differentials to estimate the error in the calculated area. (b) Estimate the percentage errors in the side and the area. 56. The side of a cube is measured to be 25 cm, with a possible error of ±1 cm. (a) Use differentials to estimate the error in the calculated volume. (b) Estimate the percentage errors in the side and volume. 57. The hypotenuse of a right triangle is known to be 10 in exactly, and one of the acute angles is measured to be 30 ◦ , with a possible error of ±1 ◦ . (a) Use differentials to estimate the errors in the sides opposite and adjacent to the measured angle. (b) Estimate the percentage errors in the sides. 58. One side of a right triangle is known to be 25 cm exactly. The angle opposite to this side is measured to be 60 ◦ , with a possible error of ±0.5 ◦ . (a) Use differentials to estimate the errors in the adjacent side and the hypotenuse. (cont.) 160 Chapter 3 / Topics in Differentiation (b) Estimate the percentage errors in the adjacent side and hypotenuse. 59. The electrical resistance R of a certain wire is given by R = k ∕ r 2 , where k is a constant and r is the radius of the wire. Assuming that the radius r has a possible error of ±5%, use differentials to estimate the percentage error in R.
  • Book cover image for: Calculus: Early Transcendentals, Metric Edition
    • James Stewart, Daniel K. Clegg, Saleem Watson, , James Stewart, James Stewart, Daniel K. Clegg, Saleem Watson(Authors)
    • 2020(Publication Date)
    Cengage Learning reserves the right to remove additional content at any time if subsequent rights restrictions require it. SECTION 14.4 Tangent Planes and Linear Approximations 979 ■ Differentials For a differentiable function of one variable, y - f s xd, we define the differential dx to be an independent variable; that is, dx can be given the value of any real number. The dif- ferential of y is then defined as 9 dy - f 9 s xd dx (See Section 3.10.) Figure 6 shows the relationship between the increment Dy and the differential dy : Dy represents the change in height of the curve y - f s xd and dy repre- sents the change in height of the tangent line when x changes by an amount dx - Dx. For a differentiable function of two variables, z - f s x, yd, we define the differentials dx and dy to be independent variables; that is, they can be given any values. Then the differential dz, also called the total differential, is defined by 10 dz - f x s x, yd dx 1 f y s x, yd dy - -z -x dx 1 -z -y dy (Compare with Equation 9.) Sometimes the notation df is used in place of dz. If we take dx - Dx - x 2 a and dy - Dy - y 2 b in Equation 10, then the differen- tial of z is dz - f x sa, bds x 2 ad 1 f y sa, bds y 2 bd So, in the notation of differentials, the linear approximation (4) can be written as f s x, yd < f sa, bd 1 dz Figure 7 is the three-dimensional counterpart of Figure 6 and shows the geometric inter- pretation of the differential dz and the increment Dz: dz represents the change in height of the tangent plane, whereas Dz represents the change in height of the surface z - f s x, yd when s x, yd changes from sa, bd to sa 1 Dx, b 1 Dyd. y x z Îx=dx 0 {a, b, f(a, b)} (a, b, 0) (a+Îx, b+Îy, 0) {a+Îx, b+Îy, f(a+Îx, b+Îy)} f(a, b) f(a, b) Îy=dy tangent plane z-f(a, b)=f x (a, b)(x-a)+f y (a, b)( y-b) surface z=f(x, y) dz Îz EXAMPLE 4 (a) If z - f s x, yd - x 2 1 3xy 2 y 2 , find the differential dz.
  • Book cover image for: Mathematical Methods for Life Sciences
    3 Applications of the Derivative
    DOI: 10.1201/9781003343288-3

    3.1 The Linear Approximation

    The concept of linear approximation is based on the geometric interpretation of the derivative. In fact, as we saw in Chapter 2 , we can view the derivative of a function f at a point, as the slope of the tangent line to the curve y = f(x) at that point. Consider a function f : D → ℝ and two points of the domain P and Q, with coordinates (x0 , f(x0 )) and (x0 + h, f(x0 + h)), respectively. We see that the line passing through the points P and Q approximates the tangent line to graph y = f(x) and also the graph itself. In particular, we get a good approximation, by choosing h very small. We emphasize once again that this is just an intuitive reasoning: only the definition of limit can rigorously account for such notions such as “near”, “approximate” and so on.
    As we see from the graph, the difference quotient
    f (
    x 0
    + h ) f (
    x 0
    )
    h
    represents the slope of the line passing through P and Q. If we consider a “small” value of h, we can effectively approximate the derivative as
    f
    (
    x 0
    )
    f (
    x 0
    + h ) f (
    x 0
    )
    h
    The symbol “≃” means that we have an approximation and not an equality.
    We obtain an estimate for the value of f(x0 + h), which is called linear approximation of f:
    f (
    x 0
    + h ) f (
    x 0
    ) +
    f
    (
    x 0
    ) h .
    (3.1)
    We can also express it more concisely as:
    Δ ( f )
    f
    (
    x 0
    ) Δ x , where Δ ( f ) = f (
    x 0
    + h ) f (
    x 0
    ) , Δ x = h .
    (3.2)
    For example, if we consider the function f(x) = 2x2 , for x0 = 1 and h = 0.02, we can write the formula (3.1) as:
    f ( 1.02 ) f ( 1 ) +
    f
    ( 1 ) 0.02 = 2 + 4 1 0.02 = 2.08
    Checking with a calculator: f(1.02) = 2 · 1.022 = 2.0808. If we choose a larger value of h, for example, h
  • Book cover image for: Calculus
    eBook - PDF

    Calculus

    Multivariable

    • Deborah Hughes-Hallett, Andrew M. Gleason, William G. McCallum(Authors)
    • 2021(Publication Date)
    • Wiley
      (Publisher)
    842 Chapter 14 DIFFERENTIATING FUNCTIONS OF SEVERAL VARIABLES Notice that the linear terms in (, ) are the same as the linear terms in (, ). The quadratic terms in (, ) can be thought of as “correction terms” to the linear approximation. (b) The contour plots of  (, ), (, ), and (, ) are in Figures 14.58–14.60. 1 −1 1 −1 2 1 0 −1 −2   Figure 14.58: Original function,  (, ) 1 −1 1 −1 2 1 0 −1 −2   Figure 14.59: Linear approximation, (, ) 1 −1 1 −1 2 1 0 −1 −2   Figure 14.60: Quadratic approximation, (, ) Notice that the contour plot of  is more similar to the contour plot of  than is the contour plot of . Since  is linear, the contour plot of  consists of parallel, equally spaced lines. An alternative, and much quicker, way to find the Taylor polynomial in the previous example is to use the single-variable approximations. For example, since cos  = 1 −  2 2! +  4 4! + ⋯ and sin  =  −  3 3! + ⋯ , we can substitute  = 2 +  and  =  +  and expand. We discard terms beyond the second (since we want the quadratic polynomial), getting cos(2 + ) = 1 − (2 + ) 2 2! + (2 + ) 4 4! + ⋯ ≈ 1 − 1 2 (4 2 + 4 +  2 ) = 1 − 2 2 − 2 − 1 2  2 and sin( + ) = ( + ) − ( + ) 3 3! + ⋯ ≈  + . Combining these results, we get cos(2 + ) + 3 sin( + ) ≈ 1 − 2 2 − 2 − 1 2  2 + 3( + ) = 1 + 3 + 3 − 2 2 − 2 − 1 2  2 . Linear and Quadratic Approximations Near (, ) The local linearization for a function  (, ) at a point (, ) is Taylor Polynomial of Degree  Approximating  (, ) for (, ) Near (, ) If  has continuous first-order partial derivatives, then  (, ) ≈ (, ) =  (, ) +   (, )( − ) +   (, )( − ). 14.7 SECOND-ORDER PARTIAL DERIVATIVES 843 This suggests that a quadratic polynomial approximation (, ) for  (, ) near a point (, ) should be written in terms of ( − ) and ( − ) instead of  and .
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