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Exercise 1.1.11 (Jordan measure and linear transformations)
Let be a linear transformation.
- (i)
- Show that there exists a non-negative real number
such that fon every elementary set
we have
(why is Jordan measurable?)
- (ii)
- Show that if
is Jordan measurable, then
is alse, and
- (iii)
- Show that .
Answers
Pick an arbitrary Jordan measurable set . By Exercise 1.1.5 this is equivalent to the fact that for any we can find two elementary sets such that
This implies
If we manage to demonstrate that and are elementary as well, with , then we are done. Thus, it suffices to prove the theorem assertion only for elementary sets. By Lemma 1.1.2 we can write represent an elementary set as a disjoint union of boxes . Knowing that a finite union of Jordan measurable sets is again Jordan measurable by Exercise 1.1.6, it is sufficient to demonstrate that is Jordan measurable for any box .
We use the strategy of expanding the proof to an always more general case with respect to the type of .
- (i)
-
is an elementary linear transformation
We have further three cases (we only consider the cases with respect to matrix rows; the cases with columns follow analogously):-
is a Type I linear transformation
In other words, exchanges any two rows of a point, and it can be represented by a matrix which is an identity matrix with rows and switched:Notice that transforms any box into another box, which is Jordan measurable; namely, it is easy to verify pointwise that
It is only left to demonstrate how changes the magnitude of the Jordan measure:
But this follows directly from the fact that only switches two intervals of ; thus, leaving the measure of unchanged. Since (Linear Algebra, Theorem 4.5), and thus .
-
is a Type II linear transformation
Now suppose that multiplies the th row of the input with a non-zero scalar , i.e.,Then it is easy to verify pointwise that
As it was in the previous case, maps a box to a box, which is Jordan measurable. We need to demonstrate the change in the magnitude of the Jordan measure:
But this follows directly from the fact that only enlarges the interval of ; thus, leaving the measure of . Since (Linear Algebra, Theorem 4.6), the assertion follows.
-
is a Type III linear transformation
In other words, adds a row of the input to its another row .In this case, does not map a box into another box; we have to improvise here. The trick is to look closer at what maps a box into (the answer is parallelepiped). If the image is Jordan measurable, then we can simply spend another and approximate this set by another elementary set from below (in case the elementary set is ) or from above (in case the elementary set is ). If we denote by an elementary linear transformation that interchanges th and th columns, then:
This representation has nice properties. Since is proven to map a Jordan measurable set to a Jordan measurable set, while preserving the original volume, it suffices to demonstrate that the set
is Jordan measurable, and has a measure equal to the original set. Knowing how Jordan measure interacts with Cartesian products from Exercise 1.1.16, it suffices to demonstrate that the parallelepiped in given by
is Jordan measurable.
Figure 1: Parrallepiped as a disjoint union of two triangles and a box, and its generalisation to higher dimensions. Assuming without loss of generality, it can be tediously verified (exercise) that a parallelepiped can be partitioned into two triangles and a box.
Since all of these figures are Jordan measurable by Exercise 1.1.8, their union must be Jordan measurable as well, and its measure is
Hence, the set
is Jordan measurable, with a measure of by Exercise 1.1.16. The rest of the proof can be finished by choosing an elementary set with covers from inner and from outer, and by adjusting accordingly.
-
- (ii)
-
is an invertible linear transformation.
By Linear Algebra, Corollary 3.6 (3), can be represented as a sequence of elementary transformations . On one hand, by Theorem 4.7 we have . On the other hand, by the previous part of this exercise , and we are done. - (iii)
- is a
linear transformation.only class of linear transformation for which the theorem
assertion is left to verify are non-invertible linear transformations. Recall from
Linear Algebra, Theorem 3.6., that using elementary linear transformations
we can
transform
into a block matrix of the form
where is an identity matrix of size , and the rest are zero matrices. The last block matrix will send any box into a lower dimensional box
and the Jordan measure of the above box is obviously zero. On one hand, applying the elementary transformations to obtain the end result will only multiply the sets Jordan measure by scaled determinants, so the result will remain zero. Hence, . On the other hand, the determinant of the non-invertible linear transformation is zero (Linear Algebra, Corollary 4.7), and we are done.
Comments
Proof. If is an elementary set, then is Jordan measurable. Indeed, recall that any invertible matrix can be written as a product of elementary operation matrices: where each is either multiplication of a row by a scalar , addition of one row to another row, or swapping of two rows. That is, is in one of the following families of matrices:
That is is obtain by multiplying the -th row of the identity matrix by is obtained by adding the -th row in the identity matrix to the -th row; is obtained by swapping the -th and -th rows of the identity matrix.
It is immediate to compute that . Also, if we have that and for , . Thus, we have that for any box , and any linear map . If is an elementary set, where are boxes, then , so is an elementary set and
Finally, if is Jordan measurable, the for any choose elementary sets such that . So, and
Taking we have that . This proves the theorem for the case that .
Now for a somewhat more cumbersome computation:
which is the Cartesian product of the parallelepiped with a box in . Indeed, if we apply to this set,
Since preserves Jordan measure (and measurability), it suffices to show the Jordan measurability of and compute its Jordan measure. By translating we may assume without loss of generality that the endpoints of are and the endpoints of are . We may also write where are right-angle triangles, with orthogonal sides parallel to the axes, and is a box, as in Figure 1 In a previous exercise it was shown that triangles are Jordan measurable. A translation of by the vector shows that has the Jordan measure of the box . Thus, is Jordan measurable and has Jordan measure , which consequently is .
We conclude that is Jordan measurable, and that , where and . Since we have just proved that for any box , the set is Jordan measurable and .
Just as for and we now use the fact that to prove the theorem for any .
Finally, if is a general invertible linear map, then where for all . So for any that is Jordan measurable, also is Jordan measurable, and thus is as well, and so on to get that is Jordan measurable. We also compute the measure by
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Comments
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You did not address the non-invertible case.isn • 2024-12-11