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If \(U\) and \(V\) are vector spaces, define the Cartesian product of \(U\) and \(V\) to be \(U \times V=\\{(\mathbf{u}, \mathbf{v}): \mathbf{u} \text { is in } U \text { and } \mathbf{v} \text { is in } V\\}\) Prove that \(U \times V\) is a vector space.

Short Answer

Expert verified
The Cartesian product \(U \times V\) satisfies all the axioms of a vector space, thus it is a vector space.

Step by step solution

01

Definition of a Vector Space

A vector space is a set of vectors along with operations of vector addition and scalar multiplication that satisfy certain axioms (closure, associativity, identity, inverse elements, distributive properties, and compatibility with scalar multiplication). To prove that \(U \times V\) is a vector space, we need to show that these axioms are satisfied for the set \(U \times V\).
02

Closure Under Addition

Consider two arbitrary elements \((u_1, v_1)\) and \((u_2, v_2)\) in \(U \times V\). The vector addition in \(U \times V\) is defined as \((u_1, v_1) + (u_2, v_2) = (u_1 + u_2, v_1 + v_2)\). Since both \(u_1 + u_2\) is in \(U\) and \(v_1 + v_2\) is in \(V\) (by the closure property of vector spaces \(U\) and \(V\)), \((u_1, v_1) + (u_2, v_2)\) is in \(U \times V\). This shows closure under addition.
03

Closure Under Scalar Multiplication

Take an arbitrary element \((u, v)\) in \(U \times V\) and a scalar \(c\). Scalar multiplication in \(U \times V\) is defined as \(c(u, v) = (cu, cv)\). Since \(cu\) is in \(U\) and \(cv\) is in \(V\) (by the closure of \(U\) and \(V\) under scalar multiplication), \(c(u, v)\) is in \(U \times V\). Hence, closure under scalar multiplication holds.
04

Associativity of Addition

For three arbitrary elements \((u_1, v_1)\), \((u_2, v_2)\), and \((u_3, v_3)\) in \(U \times V\), we verify associativity: \(((u_1, v_1) + (u_2, v_2)) + (u_3, v_3) = (u_1 + u_2, v_1 + v_2) + (u_3, v_3)\). This simplifies to \((u_1 + u_2 + u_3, v_1 + v_2 + v_3)\). Similarly, \((u_1, v_1) + ((u_2, v_2) + (u_3, v_3)) = (u_1, v_1) + (u_2 + u_3, v_2 + v_3)\), which also simplifies to \((u_1 + u_2 + u_3, v_1 + v_2 + v_3)\). Associativity holds.
05

Additive Identity

The additive identity in \(U \times V\) is \((\mathbf{0}_U, \mathbf{0}_V)\), where \(\mathbf{0}_U\) is the zero vector in \(U\) and \(\mathbf{0}_V\) is the zero vector in \(V\). For any \((u, v)\) in \(U \times V\), \((u, v) + (\mathbf{0}_U, \mathbf{0}_V) = (u + \mathbf{0}_U, v + \mathbf{0}_V) = (u, v)\), showing the presence of an additive identity.
06

Additive Inverse

For each \((u, v)\) in \(U \times V\), the additive inverse is \((-u, -v)\), since \((u, v) + (-u, -v) = (u + (-u), v + (-v)) = (\mathbf{0}_U, \mathbf{0}_V)\). Thus, an additive inverse exists for every element in \(U \times V\).
07

Distributive Properties

For scalars \(a\) and \(b\) and for any vectors \((u, v)\) and \((u', v')\) in \(U \times V\), we check the two distributive properties: 1. \(a((u, v) + (u', v')) = a(u + u', v + v') = (a(u + u'), a(v + v')) = (au + au', av + av')\). 2. \((a + b)(u, v) = ((a + b)u, (a + b)v) = (au + bu, av + bv)\), and 3. \(a(u, v) + b(u, v) = (au, av) + (bu, bv) = (au + bu, av + bv)\). These satisfy the distributive laws.
08

Compatibility of Scalar Multiplication

For scalars \(a\) and \(b\) and a vector \((u, v)\) in \(U \times V\), we need \(a(b(u, v)) = (ab)(u, v)\). Evaluating, \(a(bu, bv) = (a(bu), a(bv)) = ((ab)u, (ab)v)\), confirms compatibility with scalar multiplication.
09

Conclusion

Since the set \(U \times V\) satisfies all vector space axioms, we conclude that \(U \times V\) is indeed a vector space.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Closure Under Addition
In order to confirm that a set is a vector space, we must demonstrate that it satisfies specific criteria, one of which is closure under addition.
This property means that if you take any two elements from the set and add them together, the result should also be in the set. Let's consider two elements, \((u_1, v_1)\) and \((u_2, v_2)\), from the Cartesian product of vector spaces \(U \times V\).
According to the rules of vector addition in \(U \times V\), you add these elements component-wise: \((u_1, v_1) + (u_2, v_2) = (u_1 + u_2, v_1 + v_2)\).

Since both\(u_1 + u_2\) belongs to \(U\) and \(v_1 + v_2\) belongs to \(V\), the sum \((u_1, v_1) + (u_2, v_2)\) definitely remains in \(U \times V\).
Thus, \(U \times V\) is closed under addition, meeting this criterion of being a vector space.
Vector Space Axioms
Vector spaces are defined by several axioms that must be honored for a set to be classified as such. Let’s briefly go over what these entail in the context of \(U \times V\).

  • **Additive Identity:** There exists an additive identity, \((\mathbf{0}_U, \mathbf{0}_V)\), such that for any \((u, v)\) in \(U \times V\), we have \((u, v) + (\mathbf{0}_U, \mathbf{0}_V) = (u, v)\).
  • **Additive Inverse:** Each element \((u, v)\) has an inverse \((-u, -v)\) such that \((u, v) + (-u, -v) = (\mathbf{0}_U, \mathbf{0}_V)\).
  • **Associativity of Addition:** For any \((u_1, v_1)\), \((u_2, v_2)\), \((u_3, v_3)\), it holds that \(((u_1, v_1) + (u_2, v_2)) + (u_3, v_3) = (u_1, v_1) + ((u_2, v_2) + (u_3, v_3))\).
  • **Distributive Properties:** For scalars \(a\) and \(b\), and vectors \((u, v)\), the operations \(a((u, v) + (u', v')) = a(\mathbf{u} + \mathbf{u'}) \) and \((a + b)(u, v) = a(u, v) + b(u, v)\) hold true.
By meeting these and the additional axioms, \(U \times V\) is verified to be a vector space.
Cartesian Product
The Cartesian product is a mathematical concept that combines two sets into ordered pairs. When dealing with vector spaces \(U\) and \(V\), the Cartesian product is denoted as \(U \times V\).
It consists of all possible pairs \((\mathbf{u}, \mathbf{v})\), where \(\mathbf{u}\) is in \(U\) and \(\mathbf{v}\) is in \(V\).

In practical terms, the Cartesian product forms a new vector space, where elements are not simply numbers but pairs of vectors from each set. This structure allows us to explore and visualize relationships between vector spaces and their interactions.
In our example, proving \(U \times V\) is a vector space involves showing that this set of pairs meets all required vector space axioms.
As each of the properties and operations in \(U\) and \(V\) hold on their own, they collectively validate \(U \times V\) as a vector space.
Scalar Multiplication
Scalar multiplication is a fundamental operation in linear algebra that involves multiplying a vector by a scalar (a constant from the field over which the vector space is defined).
In \(U \times V\), let a scalar be \(c\) and consider an arbitrary vector \((u, v)\).
Scalar multiplication is defined by \(c(u, v) = (cu, cv)\).
The result \((cu, cv)\) is another element of \(U \times V\) because of the closure properties of the original vector spaces \(U\) and \(V\).
Additional important properties related to scalar multiplication for vector spaces include:
  • **Compatibility:** For any scalars \(a\) and \(b\), \(a(b(u, v)) = (ab)(u, v)\).
  • **Distributive over Vectors and Scalars:** \(a((u, v) + (u', v')) = a(u, v) + a(u', v')\) and \((a + b)(u, v) = a(u, v) + b(u, v)\).
Through these properties, scalar multiplication not only demonstrates closure but also interacts reliably with addition within \(U \times V\), reinforcing the vector space structure.

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Most popular questions from this chapter

A pendulum consists of a mass, called a bob, that is affixed to the end of a string of length \(L\) (see Figure 6.26 ). When the bob is moved from its rest position and released, it swings back and forth. The time it takes the pendulum to swing from its farthest right position to its farthest left position and back to its next farthest right position is called the period of the pendulum. (Figure can't copy) Let \(\theta=\theta(t)\) be the angle of the pendulum from the vertical. It can be shown that if there is no resistance, then when \(\theta\) is small it satisfies the differential equation \\[ \theta^{\prime \prime}+\frac{g}{L} \theta=0 \\] where \(g\) is the constant of acceleration due to gravity, approximately \(9.7 \mathrm{m} / \mathrm{s}^{2}\). Suppose that \(L=1 \mathrm{m}\) and that the pendulum is at rest (i.e., \(\theta=0\) ) at time \(t=0\) second. The bob is then drawn to the right at an angle of \(\theta_{1}\) radians and released. (a) Find the period of the pendulum. (b) Does the period depend on the angle \(\theta_{1}\) at which the pendulum is released? This question was posed and answered by Galileo in \(1638 .\) [Galileo Galilei \((1564-1642)\) studied medicine as a student at the University of Pisa, but his real interest was always mathematics. In \(1592,\) Galileo was appointed professor of mathematics at the University of Padua in Venice, where he taught primarily geometry and astronomy. He was the first to use a telescope to look at the stars and planets, and in so doing, he produced experimental data in support of the Copernican view that the planets revolve around the sun and not the earth. For this, Galileo was summoned before the Inquisition, placed under house arrest, and forbidden to publish his results. While under house arrest, he was able to write up his research on falling objects and pendulums. His notes were smuggled out of Italy and published as Discourses on Two New Sciences in 1638.]

The set of all linear transformations from a vector space \(V\) to a vector space \(W\) is denoted by \(\mathscr{L}(V, W)\). If \(\operatorname{sand}\) T are \(\operatorname{in} \mathscr{L}(V, W),\) we can define the sum \(S+T\) of \(S\) and \(T b y\) \\[ (S+T)(\mathbf{v})=S(\mathbf{v})+T(\mathbf{v}) \\] for all \(\mathbf{v}\) in \(V\). If \(c\) is a scalar, we define the scalar multiple \(c T\) of Thy cto be \\[ (c T)(\mathbf{v})=c T(\mathbf{v}) \\] for all \(\mathbf{v}\) in \(V\). Then \(S+T\) and \(c\) T are both transformations from \(V\) to \(W\) Prove that \(S+T\) and \(c T\) are linear transformations.

Determine whether the set \(\mathcal{B}\) is a basis for the vector space \(V\) $$V=\mathscr{P}_{2}, \mathcal{B}=\left\\{x, 1-x, 1+x+x^{2}\right\\}$$

Show that \(T: \mathscr{P}_{n} \rightarrow \mathscr{P}_{n}\) defined by \(T(p(x))=p(x-2)\) is an isomorphism.

Find the dimension of the vector space \(V\) and give a basis for \(V\) \(V=\left\\{A \text { in } M_{22}: A \text { is upper triangular }\right\\}\)

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