Question

Show that the Lie derivative \(\mathcal{L}_{x}\) commules with all operations of contraction \(C_{t}^{y}\) on a tensor field \(T\), $$ \mathcal{L}_{X} C_{J} T=C_{j} \mathcal{L}_{\mathrm{Y}} T $$

Short answer

Therefore, it's proven that the Lie derivative \(\mathcal{L}\) commutes with all operations of contraction \(C_{J}\) on a tensor field \(T\).

Step-by-step solution

Definition of the Lie derivative

The Lie derivative \(\mathcal{L}_X\) of a tensor field T in direction X is given by the limit: \[ \mathcal{L}_XT = \lim_{t→0} \frac{\phi_t^*T - T}{t} \] Where \(\phi_t\) is the flow of X

Apply contraction to both sides of the Lie derivative definition

Now apply contraction \(C_J\) to both sides of this definition to get: \[ C_J(\mathcal{L}_XT) = \lim_{t→0} \frac{C_J(\phi_t^*T - T)}{t} \]

Applying the Leibnitz rule

Now, we can apply the Leibnitz rule (which states that contraction operations distribute over addition and scale with scalar multiplication) on the right hand side of this equation: \[ C_J(\mathcal{L}_XT) = \lim_{t→0} \frac{C_J(\phi_t^*T)-C_J(T)}{t} \]

Recognizing the Lie derivative

Now one can observe that the right hand side is just the definition of the Lie derivative applied to contraction of the tensor field \(T\), hence: \[ C_J(\mathcal{L}_XT) = \mathcal{L}_X(C_JT) \]

Key concepts

Tensor Fields

In the realm of differential geometry, understanding what tensor fields are is crucial. A tensor field can be thought of as a generalization of scalar and vector fields. Essentially, it assigns a tensor to each point in a given space, enabling it to describe more complex geometrical and physical systems.
They can vary in rank, dimension, and the type of space they are applied to. When examining physical phenomena, tensor fields can represent everything from simple lengths and areas to complex stress and energy distributions.
To grasp the concept, one can consider vectors, which are simple tensors of rank 1, that assign a direction and magnitude to points in space. In more complex cases, a tensor field might describe flows or fields where both magnitude and direction can change from point to point.

• Tensors of rank 0: Scalars
• Tensors of rank 1: Vectors
• Tensors of rank 2 or higher: Matrices and beyond

The structure provided by a tensor field forms the backbone for much of modern physics and engineering, allowing for a detailed and comprehensive modeling of various fields such as electromagnetism and general relativity.

Contraction Operation

The contraction operation in the context of tensors is a significant concept as it deals with reducing the rank of a tensor by pairing and summing over one covariant and one contravariant index. This operation helps in simplifying tensor expressions and is critical in the manipulation and application of tensor equations.
For example, starting with a tensor of rank 2, applying contraction results in a scalar by summing over a specific pair of indices.

• This is similar to taking the trace of a matrix, where the diagonal elements are summed up.
• In a rank 3 tensor, contraction reduces it to a rank 1 tensor or vector.

Understanding contraction not only simplifies complex tensor calculus but also plays a vital role in the computation of the Lie derivative, where operations must be commuted and simplified for ease of calculation.
In practical applications, contractions are frequently used in physics to compute invariant quantities, especially within the formulation of theories like general relativity, helping to describe phenomena in a coordinate-free manner.

Leibnitz Rule

The Leibnitz rule is essential to the calculation involving derivatives of tensor operations, including the contraction of tensors. It is named after the mathematician Gottfried Wilhelm Leibniz and encapsulates the distributive properties of derivative operations.

• In essence, it states that the derivative of a product is the sum of the derivative of the first factor times the second, plus the first factor times the derivative of the second.
• Mathematically, for scalars, it can be expressed as \((f \, g)' = f' \, g + f \, g'\).

When applied to tensors, the Leibnitz rule principles extend to show that the derivative operation will distribute over any sum or difference within the contraction operation. This effectively simplifies the complex algebra involved in deriving commutation properties of operations such as the Lie derivative.
Having a firm grasp of the Leibnitz rule in tensor calculus is particularly beneficial in the study of differential geometry. It aids in understanding how changes in tensor fields translate and interact under different transformations and operations within the context of manifold theory.