Exercise 1.1.10 (Balls are Jordan measurable)

Let B(y,r) = {x d : x y < r} be an open ball, and let B(y,r)¯ = {x d : x y r} be a closed ball.

(i)
Show that balls are Jordan measurable, with the Jordan measure mJ(B) = cd rd

for some constant c(d) depending only on the dimension d.

(ii)
Establish the crude bounds ( 2 d )d c d 2d

Answers

(i) Jordan measurability.
First note that by translation invariance of Jordan measure (Exercise 1.1.6) we can simpy look at the ball B(0,r) = B(y,r) y centered at the origin. Furthermore, we will look at the upper half-ball B+ := B(0,r) (d1 × +), since the identical proof for the lower half-ball B = B(0,r) (d1 × ) will give us the same formula, and by disjunction property B(0,r) = B(0,r) B+(0,r) we can simply sum up the measures of both halves.

Proof. We will use the same strategy that we used in the previous exercises, i.e., we will try to represent the figure in some functional way, so that we can easily estimate its measure numerically und then simply apply Exercise 1.1.7. The function describing the shape of an upper half-ball is

f : Bd1(0,r) (x 1,,xd1)r2 (x1 , , xd1 )2

In other words, we demonstrate that the area under the graph of the above function is the upper-ball we are looking at

B(0,r) (d1 × +) = {(x,xd) d : x Bd1(0,r), 0 x d f(x)}

This is easy to verify. Pick an arbitrary x A(f). Then,

x = i=1dxi2 = i=1d1xi2 + xd2 i=1d1xi2 + r2 (x1,,xd1)2 = r

Since also xd 0, we have x B+(0,r). Conversely, let x B+(0,r). Then from i=1dxi2 < r both conditions i=1d1xi2 < r and xd2 < r2 i=1d1xi2 = f2(x1,,xd) follow. Similarly we can prove that the lower half-ball is the area under the graph of f.
Using this result, we want to demonstrate that Bd(0,r) is Jordan measurable. If we knew that Bd1(0,r) is Jordan measurable, it could be possible to show that Bd(0,r) is Jordan measurable by showing that the area under f is Jordan measurable. This is obviously an induction matter.

  • Induction basis. Suppose that d = 2. Then Bd1(0,r) is simply an interval [r,r]. But it is also a compact box; thus, by Exercise 1.1.7 the area under f must be Jordan measurable.
  • Induction step. Now suppose inductively that we have proven this statement for some d 1 > 2; we demonstrate that this implies that the statement is also true for d. In other words, assume that Bd1(0,r) is Jordan measurable. We demonstrate the Jordan measurability of Bd(0,r) by the criteria (3) from the Exercise 1.1.5. Thus, pick an arbitrary 𝜖 > 0. By Exercise 1.1.5 applied to the previous dimension, we can find an outer cover Bd1¯𝜖 and an inner cover Bd1̲𝜖 of Bd1(0,r) such that m (Bd1¯𝜖Bd1¯𝜖) < 𝜖 r. Note that since Bd1̲𝜖 Bd1¯𝜖 we can represent the outer cover as the union of the inner cover with the cover of the "boundary":

    Bd1¯𝜖 = Bd1̲ 𝜖 (Bd1¯𝜖Bd1̲𝜖)

    By Exercise 1.1.1 both parts are elementary. At last, by Lemma 1.1.2 we can represent both inner and outer cover as the union of disjoint boxes. However, it will be very helpful later in the proof if we know that the boxes of which this elementary set consists are not longer than (𝜖mJ (B(d1)(0,r)))2 1 2r in each co-ordinate. In other words, select n : 2r n < (𝜖mJ (B(d1)(0,r)))2 1 2r and using the usual procedure partition the box [r,r]d1 as

    G := { [r + 2r n k1,r + 2r n k1 + 2r n ] × × [r + 2r n kd1,r + 2r n kd1 + 2r n ] : k d,0 k i < n}

    Then considering the collection of disjoint boxes in the inner and outer cover we take a common refinement, and the refined subsets will then be again elementary can be represented as disjoint boxes. We index this disjoint boxes, which have vertices shorter than (𝜖mJ (B(d1)(0,r)))2 1 2r, from 1 to Z :

    {B Bd1(0,r)̲}##G = { [a i(1),b i(1)] × [a i(d1),b i(d1)] : i = 1z} {B Bd1(0,r)¯}##G = { [ai(1),b i(1)] × [a i(d1),b i(d1)] : i = 1,,z} { [ai(1),b i(1)] × [a i(d1),b i(d1)] : i = z + 1,,Z}

    Using both, we now try to cover the area under the function f on Bd1(0,r).

    Remark 1. Let E = i=1d1[ai,bi] be some box in Bd1(0,r). Then f will achieve its maximum and its minimum on the edges of E.

    Proof. First notice that f is monotonically decreasing with respect to the norm, i.e., x,y Bd1(0,r) : xyf(x) f(y). Thus, we simply need to prove that some of the edges of E have the lowest norm. Pick an arbitrary x E. Since x = (x1,,xd1) we have ai xi bi in every co-ordinate. This implies, xi2 max {ai2,bi2} =: li2 and accordingly x = i=1d1xi2 i=1d1li2 = l where l is an edge of E. Thus, l has the lowest norm in E (obviously, it may not be unique). Similarly, some edge h of E has the highest norm in E. □

    Remark 2. Now consider the maximal difference between f values on E = i=1d1[ai,bi]. By monotonicity, we equivalently look at the biggest difference in norms of the points in E:

    x,y E : x2 y2 h2 l2 = i=1d1 max {a i2,b i2} i=1d1 min {a i2,b i2} = i=1d1|b i2 a i2| = i=1d1|(b i ai)(bi + ai)|.

    Notice that in our case bi ai 2rn (𝜖mJ (B(d1)(0,r)))2 1 2r and |bi + ai| 2r; thus, the above term will never exceed (𝜖mJ (B(d1)(0,r)))2. Furthermore, for xy we have

    f(y) f(x) = r2 y2 r2 x2 r2 y2 r2 + x2 = x2 y2 𝜖 mJ (B(d1)(0,r)).

    We now use these observations to construct outer and inner covers. By Remark 1, the highest/lowest point on a box i is some hili:

    Bd(0,r)̲ 𝜖 = i=1z [a i(1),b i(1)] × [a i(d1),b i(d1)] × [0,f (h i)] Bd(0,r)¯𝜖 = ( i=1z [a i(1),b i(1)] × [a i(d1),b i(d1)] × [0,f(l i)]) ( i=z+1Z [a i(1),b i(1)] × [a i(d1),b i(d1) × [0,f(l i)]])

    Then, by properties of elementary measure, the difference in the measure of the outer and the inner cover can be calculated as follows. By Remark 2, the maximum difference between the values of f on a single box cannot exceed 𝜖, and f is obviously bounded by r. Thus,

    m (Bd(0,r)¯𝜖 Bd(0,r)̲ 𝜖) = i=1n j=1d1 [b i(j) a i(j)] f (l i) + i=z+1Z j=1d1 [b i(j) a i(j)] f (l i) i=1z j=1d1 [b i(j) a i(j)] f (h i) = i=1z j=1d1 [b i(j) a i(j)] (f (l i) f (hi)) + i=n+1Z j=1d1 [b i(j) a i(j)] f (l i) i=1z j=1d1 [b i(j) a i(j)] 𝜖 mJ (B(d1)(0,r)) + i=n+1Z j=1d1 [b i(j) a i(j)] r = 𝜖 mJ (B(d1)(0,r)) m (B(d1)(0,r)̲) + r m (Bd1¯𝜖Bd1̲ 𝜖) 𝜖 + 𝜖 = 2𝜖.

    Since our choice of 𝜖 was arbitrary, by Exercise 1.1.5 B(d)(0,r) must be Jordan measurable. This closes the induction.

(ii) Bounds for the volume formula.

Proof. To establish the bounds, note the basic relationship

[ r d, r d ]d B(d)(0,r) [r,r]d.

PIC PIC
Figure 1: Inscribing a cube into a ball in R2 (left) and R3 (right). If the main diagonal of the cube is to be equivalent to the ball diameter of 2r, then the sides must be of length 2r or 23r respectively.

To see why, pick an arbitrary x [ r d, r d ]d. Then, x2 = i=1dxi2 i=1dr2 d = r2; thus x B(d)(0,r). Similarly pick an arbitrary x B(d)(0,r). Then

x = i=1dxi2 ri = 1,,d : xi2 r2i = 1,,d : x i [r,r].

By monotonicity of Jordan measure (Exercise 1.1.6):

m ( [ r d, r d ]) m (B(d)(0,r)) m ( [r,r]d)

Evaluating these elementary measures we obtain:

( 2 d )d rd m (B(d)(0,r)) (2d) rd

as desired. □

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2020-03-16 00:00
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