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Exercise 1.1.10 (Balls are Jordan measurable)
Let be an open ball, and let be a closed ball.
- (i)
- Show that balls are Jordan measurable, with the Jordan measure
for some constant depending only on the dimension .
- (ii)
- Establish the crude bounds
Answers
(i) Jordan measurability.
First note that by translation invariance of Jordan measure (Exercise 1.1.6) we can simpy
look at the ball
centered at the origin. Furthermore, we will look at the upper half-ball
, since the identical proof
for the lower half-ball
will give us the same formula, and by disjunction property
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
In other words, we demonstrate that the area under the graph of the above function is the upper-ball we are looking at
This is easy to verify. Pick an arbitrary . Then,
Since also ,
we have .
Conversely, let .
Then from both
conditions
and
follow. Similarly we can prove that the lower half-ball is the area under the graph
of .
Using this result, we want to demonstrate that
is Jordan measurable.
If we knew that
is Jordan measurable, it could be possible to show that
is Jordan measurable by showing that the area under
is
Jordan measurable. This is obviously an induction matter.
- Induction basis. Suppose that . Then is simply an interval . But it is also a compact box; thus, by Exercise 1.1.7 the area under must be Jordan measurable.
-
Induction step. Now suppose inductively that we have proven this statement for some ; we demonstrate that this implies that the statement is also true for . In other words, assume that is Jordan measurable. We demonstrate the Jordan measurability of by the criteria (3) from the Exercise 1.1.5. Thus, pick an arbitrary . By Exercise 1.1.5 applied to the previous dimension, we can find an outer cover and an inner cover of such that . Note that since we can represent the outer cover as the union of the inner cover with the cover of the "boundary":
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 in each co-ordinate. In other words, select and using the usual procedure partition the box as
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 , from to :
Using both, we now try to cover the area under the function on .
Proof. First notice that is monotonically decreasing with respect to the norm, i.e., . Thus, we simply need to prove that some of the edges of have the lowest norm. Pick an arbitrary . Since we have in every co-ordinate. This implies, and accordingly where is an edge of . Thus, has the lowest norm in (obviously, it may not be unique). Similarly, some edge of has the highest norm in . □
Remark 2. Now consider the maximal difference between values on . By monotonicity, we equivalently look at the biggest difference in norms of the points in :
Notice that in our case and ; thus, the above term will never exceed . Furthermore, for we have
We now use these observations to construct outer and inner covers. By Remark 1, the highest/lowest point on a box is some :
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 on a single box cannot exceed , and is obviously bounded by . Thus,
Since our choice of was arbitrary, by Exercise 1.1.5 must be Jordan measurable. This closes the induction.
(ii) Bounds for the volume formula.
Proof. To establish the bounds, note the basic relationship
To see why, pick an arbitrary . Then, ; thus . Similarly pick an arbitrary . Then
By monotonicity of Jordan measure (Exercise 1.1.6):
Evaluating these elementary measures we obtain:
as desired. □