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Introduction

The mathematical idea of a vector plays an important role in many areas of physics.

  • Thinking about a particle traveling through space, we imagine that its speed and direction of travel can be represented by a vector v in 3-dimensional Euclidean space R3. Its path in time t might be given by a continuously varying line — perhaps with self-intersections — at each point of which we have the velocity vector v(t).
  • A static structure such as a bridge has loads which must be calculated at various points. These are also vectors, giving the direction and magnitude of the force at those isolated points
  • In the theory of electromagnetism, Maxwell’s equations deal with vector fields in 3-dimensional space which can change with time. Thus at each point of space and time, two vectors are specified, giving the electrical and the magnetic fields at that point.
  • Given two different frames of reference in the theory of relativity, the transformation of the distances and times from one to the other is given by a linear mapping of vector spaces.
  • In quantum mechanics, a given experiment is characterized by an abstract space of complex functions. Each function is thought of as being itself a kind of vector. So we have a vector space of functions, and the methods of linear algebra are used to analyze the experiment.

Looking at these five examples where linear algebra comes up in physics, we see that for the first three, involving “classical physics”, we have vectors placed at different points in space and time. On the other hand, the fifth example is a vector space where the vectors are not to be thought of as being simple arrows in the normal, classical space of everyday life. In any case, it is clear that the theory of linear algebra is very basic to any study of physics.

But rather than thinking in terms of vectors as representing physical processes, it is best to begin these lectures by looking at things in a more mathematical, abstract way. Once we have gotten a feeling for the techniques involved, then we can apply them to the simple picture of vectors as being arrows located at different points of the classical 3-dimensional space.

Question for Linear Algebra and Matrices - Mathematical Methods of Physics, UGC - NET Physics
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In which area of physics do Maxwell's equations deal with vector fields?
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Basic Definitions 

Let X and Y be sets. The Cartesian product X × Y , of X with Y is the set of all possible pairs (x, y ) such that x ∈ X and y ∈ Y .


A group is a non-empty set G, together with an operation, which is a mapping ‘ · ’ : G × G → G, such that the following conditions are satisfied.

1. For all a, b, c ∈ G, we have (a · b) · c = a · (b · c),

2. There exists a particular element (the “neutral” element), often called e in group theory, such that e · g = g · e = g, for all g ∈ G.

3. For each g ∈ G, there exists an inverse element g−1 ∈ G such that g · g−1 = g−1 · g = e.

If, in addition, we have a · b = b · a for all a, b ∈ G, then G is called an “Abelian” group.


 A field is a non-empty set F, having two arithmetical operations, denoted by ‘+’ and ‘·’, that is, addition and multiplication. 

Under addition, F is an Abelian group with a neutral element denoted by ‘0’. Furthermore, there is another element, denoted by ‘1’, with 1 0, such that F \ {0} (that is, the set F, with the single element 0 removed) is an Abelian group, with neutral element 1, under multiplication. In addition, the distributive property holds:

a · (b + c) = a · b + a · c and (a + b) · c = a · c + b · c, for all a, b, c ∈ F .

The simplest example of a field is the set consisting of just two elements {0, 1} with the obvious multiplication. This is the field Z/2Z. Also, as we have seen in the analysis lectures, for any prime number p ∈ N, the set Z/pZ of residues modulo p is a field.


The following theorem, which should be familiar from the analysis lectures, gives some elementary general properties of fields.

Theorem 1. Let F be a field. Then for all a, b ∈ F, we have:

1. a · 0 = 0 · a = 0,

2. a · (−b) = −(a · b) = (−a) · b,

3. −(−a) = a,

4. (a−1)−1 = a, if a 0,

5. (−1) · a = −a,

6. (−a) · (−b) = a · b,

7. a · b = 0 ⇒ a = 0 or b = 0.

 

Proof. An exercise 

So the theory of abstract vector spaces starts with the idea of a field as the underlying arithmetical system. But in physics, and in most of mathematics (at least the analysis part of it), we do not get carried away with such generalities.
Instead we will usually be confining our attention to one of two very particular fields, namely either the field of real numbers R, or else the field of complex numbers C.

Despite this, let us adopt the usual generality in the definition of a vector space.

 A vector space V over a field F is an Abelian group — with vector addition denoted by v + w, for vectors v, w ∈ V. The neutral element is the “zero vector” 0. Furthermore, there is a scalar multiplication F × V → V satisfying (for arbitrary a, b ∈ F and v, w ∈ V):

1. a · (v + w) = a · v + a · w,
2. (a + b) · v = a · v + b · v,
3. (a · b) · v = a · (b · v), and
4. 1 · v = v for al l v ∈ V.

Examples

  • Given any field F, then we can say that F is a vector space over itself. The vectors are just the elements of F . Vector addition is the addition in the field.

Scalar multiplication is multiplication in the field.

  • Let Rn  be the set of n-tuples, for some Linear Algebra and Matrices - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET That is, the set of ordered lists of n real numbers. One can also say that this is

Linear Algebra and Matrices - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET

the Cartesian product, defined recursively. Given two elements

(x1 , ... , xn ) and (y1, ... , yn)

in Linear Algebra and Matrices - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET , then the vector sum is simply the new vector

(x1 + y1, ... , xn + yn).

Scalar multiplication is

a · (x1, ... , xn) = (a · x1, ... , a · xn).

It is a trivial matter to verify that Linear Algebra and Matrices - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET, with these operations, is a vector space over Linear Algebra and Matrices - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET

  • Let C0 ([0, 1], Linear Algebra and Matrices - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET be the set of all continuous functions f : [0, 1] → Linear Algebra and Matrices - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET This is a vector space with vector addition

(f + g)(x) = f (x) + g(x),

for all x ∈ [0, 1], defining the new function (f + g) ∈ C0([0, 1], Linear Algebra and Matrices - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET for all f , g ∈ C0([0, 1], Linear Algebra and Matrices - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET Scalar multiplication is given by

(a · f )(x) = a · f (x)

for all x ∈ [0, 1].

Question for Linear Algebra and Matrices - Mathematical Methods of Physics, UGC - NET Physics
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Which of the following statements is true about a group?
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Subspaces

Let V be a vector space over a field F and let W ⊂ V be some subset. If W is itself a vector space over F , considered using the addition and scalar multiplication in V, then we say that W is a subspace of V. Analogously, a subset H of a group G, which is itself a group using the multiplication operation from G, is called a subgroup of G. Subfields are similarly defined.


Theorem 2. Let W ⊂ V be a subset of a vector space over the field F .

Then W is a subspace of V ⇔ a · v + b · w ∈ W,

for all v, w ∈ W and a, b ∈ F .

Proof. The direction ‘⇒’ is trivial.

For '⇐,’, begin by observing that 1. v + 1.w= v+w ∈ W, and a.v+0.w = a.v ∈ W, for all v, w ∈ W and a ∈ F. Thus W is closed under vector addition and scalar multiplication. 

Is W a group with respect to vector addition? We have 0.v= 0 ∈ W, for v ∈ W; therefore the neutral element 0 is contained in W. For an  arbitrary v ∈ W we have

 v + (−1) · v = 1 · v + (−1) · v
= (1 + (−1)) · v
= 0 · v
= 0.

Therefore (−1) · v is the inverse element to v under addition, and so we can simply write  (-1) .v = -v. the other axioms for a vector space can be easily checked.

The method of this proof also shows that we have similar conditions for subsets of groups or fields to be subgroups, or subfields, respectively. 

The document Linear Algebra and Matrices - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET is a part of the Physics Course Physics for IIT JAM, UGC - NET, CSIR NET.
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FAQs on Linear Algebra and Matrices - Mathematical Methods of Physics, UGC - NET Physics - Physics for IIT JAM, UGC - NET, CSIR NET

1. What are subspaces in linear algebra?
Ans. In linear algebra, a subspace is a subset of a vector space that satisfies the three conditions of being closed under addition, closed under scalar multiplication, and contains the zero vector. Subspaces are essential in linear algebra as they help in understanding the structure and properties of vector spaces.
2. What is the difference between a subspace and a span in linear algebra?
Ans. A subspace is a subset of a vector space that satisfies the three conditions of being closed under addition, closed under scalar multiplication, and contains the zero vector. On the other hand, a span is a set of all possible linear combinations of a given set of vectors. The span of a set of vectors may or may not be a subspace, depending on whether it satisfies the three conditions of being closed under addition, closed under scalar multiplication, and contains the zero vector.
3. How do you determine if a set of vectors forms a subspace?
Ans. To determine if a set of vectors forms a subspace, we need to check if it satisfies the three conditions of being closed under addition, closed under scalar multiplication, and contains the zero vector. This can be done by taking any two vectors from the set and adding them, checking if the sum is still in the set. Similarly, we can take any vector from the set and multiply it by a scalar, checking if the product is still in the set. Finally, we need to check if the zero vector is in the set.
4. What is the role of subspaces in solving systems of linear equations?
Ans. Subspaces play a crucial role in solving systems of linear equations as they help in determining the solutions of the system. The solutions of a system of linear equations can be found by finding the intersection of the subspaces spanned by the coefficient matrix and the constant vector. If the intersection is non-empty, then the system has a unique solution, and if the intersection is empty, then the system has no solution.
5. Can a subspace have infinitely many vectors?
Ans. Yes, a subspace can have infinitely many vectors, as long as it satisfies the three conditions of being closed under addition, closed under scalar multiplication, and contains the zero vector. For example, the subspace of all polynomials of degree at most n, where n is a positive integer, contains infinitely many vectors.
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