Tensors Explained Intuitively: Covariant, Contravariant, Rank
TLDRThe script explores the concept of tensors as fundamental to understanding Einstein's General Relativity, especially the curvature of spacetime. It explains tensors as mathematical objects that transform with basis vector changes, distinguishing between contra-variant and co-variant components. The script illustrates how tensors of different ranks associate numbers with combinations of basis vectors, highlighting the creation of rank 2 tensors through various component multiplications, emphasizing the consistent transformation of tensor components with basis changes.
Takeaways
- π Tensors are fundamental to understanding the curvature of spacetime in Einstein's General Relativity.
- π A tensor of rank 1 is essentially a vector, which can be described in two ways: contra-variant and co-variant components.
- π Contra-variant components of a vector decrease when the basis vectors' lengths are increased, and vice versa.
- π Co-variant components, on the other hand, increase or decrease in tandem with the lengths of the basis vectors.
- π The distinction between contra-variant and co-variant components is marked by the use of super-scripts for the former and sub-scripts for the latter.
- π§ The same vector can be described using either contra-variant or co-variant components, but the two are not interchangeable.
- π Tensors of higher rank, such as rank 2, can be created by combining components of vectors in various ways, including contra-variant and co-variant combinations.
- π A rank 2 tensor can be represented with two contra-variant indices, one co-variant and one contra-variant index, or two co-variant indices.
- π The essence of a tensor is its transformation properties under a change of basis, which must adhere to specific rules to qualify as a tensor.
- π Tensors are not limited to being constructed from vector components; they can represent more complex relationships between basis vectors.
- π In tensors of higher ranks, such as rank 3, numbers are associated with combinations of three basis vectors, allowing for intricate descriptions of spatial relationships.
Q & A
What are tensors in the context of mathematics and physics?
-Tensors are mathematical objects that describe the transformation properties when the basis vectors change. They are crucial for understanding concepts such as the curvature of space-time in Einstein's General Relativity.
What is the relationship between a tensor of rank 1 and a vector?
-A tensor of rank 1 is essentially a vector. It has components that are associated with each of the basis vectors in the vector space.
How are vectors typically described in terms of basis vectors?
-Vectors are typically described by the number of each basis vector needed to add together to produce it, which are known as the vector's components.
What is the alternative way to describe a vector in terms of basis vectors?
-An alternative way to describe a vector is by taking the dot product of the vector with each of the basis vectors.
What happens to the components of a vector when the lengths of the basis vectors are doubled?
-When the lengths of the basis vectors are doubled, the components of the vector decrease, illustrating the concept of contra-variant components.
What is the term used to describe the components of a vector that decrease when the basis vectors' lengths increase?
-These components are referred to as 'contra-variant' components of the vector.
How are 'co-variant' components different from 'contra-variant' components?
-Co-variant components are those that increase or decrease in the same way as the lengths of the basis vectors change, in contrast to contra-variant components which change in the opposite manner.
How can we distinguish between 'co-variant' and 'contra-variant' components in notation?
-Co-variant components are usually denoted with subscript indices, while contra-variant components are denoted with superscript indices.
What is a tensor of rank 2 and how is it related to vectors?
-A tensor of rank 2 is an object that can be created by multiplying components of two vectors together in various combinations of contra-variant and co-variant indices. It generalizes the concept of a matrix to a higher-dimensional space.
How does the rank of a tensor relate to the number of basis vectors it associates with?
-The rank of a tensor indicates the number of basis vectors it associates with. For example, a tensor of rank 1 associates a number with each basis vector, while a tensor of rank 2 associates a number with every combination of two basis vectors.
Can tensors be created from anything other than vector components?
-Yes, tensors do not necessarily have to be created from vector components. They can represent a wide range of mathematical and physical quantities that transform in a specific way under changes of basis.
Outlines
π Understanding Tensors and Their Transformations
This paragraph introduces tensors as mathematical objects that change in a specific way when the basis vectors are altered. It emphasizes the importance of understanding tensors for grasping the concept of space-time curvature in Einstein's General Relativity. The paragraph explains the concept of a tensor of rank 1, which is essentially a vector, and how it can be described using either the typical method of listing components or through dot products with basis vectors. The distinction between 'contra-variant' and 'co-variant' components is made clear, with the former decreasing when basis vectors' lengths increase and vice versa, while the latter varies directly with the lengths of the basis vectors. The paragraph also explains how to denote these components differently using subscripts and superscripts and highlights the importance of consistent naming for vectors regardless of changes in basis vectors.
π Exploring Higher Rank Tensors and Their Compositions
The second paragraph delves into higher rank tensors, specifically rank 2, and how they can be formed by multiplying components of vectors in various combinations, resulting in different matrices that represent the same tensor but with different types of index valuesβ'contra-variant' and 'co-variant'. It illustrates that a tensor's nature is defined by how its components transform with the change in basis vectors, similar to the objects described in the paragraph. The concept extends beyond vectors, as tensors of rank 2 associate numbers with combinations of two basis vectors, and tensors of rank 3 associate numbers with combinations of three. The paragraph concludes by noting that tensors can be composed of combinations of components from multiple vectors and that different descriptions of a tensor can be created by varying the use of contra-variant and co-variant index values.
Mindmap
Keywords
π‘Tensors
π‘Curvature of Spacetime
π‘Rank of a Tensor
π‘Basis Vectors
π‘Contra-variant Components
π‘Co-variant Components
π‘Dot Product
π‘Index Values
π‘Tensor of Rank 2
π‘Transformation
π‘Vector Components
Highlights
Tensors are fundamental to understanding the curvature of space-time in Einsteinβs General Relativity.
A tensor of rank 1 is equivalent to a vector.
Vectors can be described using the basis vectors or through dot products with them.
The components of a vector decrease when the basis vectors' lengths are increased.
Contra-variant components of a vector change inversely to the basis vectors' length.
Co-variant components of a vector change directly with the basis vectors' length.
Different notations are used for co-variant and contra-variant components to distinguish them.
The same vector can be described using different components based on the basis vectors' lengths.
Tensors of rank 2 can be represented as matrices formed by multiplying contra-variant components of different vectors.
A rank 2 tensor can have mixed index values of co-variant and contra-variant components.
Tensors can also be described using only co-variant components.
The transformation properties of tensor components are key to their definition.
Tensors are not limited to being created from vector components.
A tensor of rank 1 associates a number with each basis vector.
In a rank 2 tensor, a number is associated with every combination of two basis vectors.
A rank 3 tensor involves associating numbers with combinations of three basis vectors.
Rank 3 tensors can be composed of combinations of components from three vectors with various index value combinations.
Transcripts
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