Are Lie Brackets and Their Derivatives Equivalent in Vector Field Calculations?

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In summary, when asked to prove the equation \mathcal{L}_{u}\mathcal{L}_{v}W - \mathcal{L}_{v}\mathcal{L}_{u}W = \mathcal{L}_{[u,v]}, the individual was able to simplify and expand using scalar linearity to arrive at the solution [u,v]w. However, they were unsure if this was equivalent to the given equation. In the second question, the individual was asked to calculate the Lie bracket [X,Y] and determine if it was equivalent to a given equation involving derivatives. They were able to solve it and also realized they had left out a vector field in the right-hand side of the first equation.
  • #1
pleasehelpmeno
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Hi i have two questions:
1) When asked to prove [itex]\mathcal{L}_{u}\mathcal{L}_{v}W - \mathcal{L}_{v}\mathcal{L}_{u}W = \mathcal{L}_{[u,v]}[/itex].

I achieved [itex][u,v]w = \mathcal{L}_{[u,v]}[/itex]. This was found by appliying a scalar field <b> to the LHS and simplifying and expanding using + and scalar linearitys to get [itex][u,v]w[/itex] but I am not sure if these are equivalent.

2) When asked to calculate the Lie bracket [X,Y] where [itex]X=5x^{2}\frac{\partial}{\partial t}-4t\frac{\partial}{\partial x} [/itex] and [itex]Y= y\frac{\partial}{\partial t} + t\frac{\partial}{\partial y} [/itex] is this equivalent to:
[itex]\left((5x^{2}\frac{\partial}{\partial t} -4t\frac{\partial}{\partial x})\frac{\partial (y\frac{\partial}{\partial t} + t\frac{\partial}{\partial y})}{\partial x^{a}}-(y\frac{\partial}{\partial t} + t\frac{\partial}{\partial y})\frac{\partial (5x^{2}\frac{\partial}{\partial t}-4t\frac{\partial}{\partial x})}{\partial x}\right)\frac{\partial}{\partial x^{b}} [/itex]

and if so can it be expanded any further I am not so sure but i don't fully understand [itex] \frac{\partial}{\partial x^{a}} [/itex] derivatives.
 
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  • #2
never mind figured it out
 
  • #3
I'm sure you're missing out the vector field W in the RHS of 1).
 
  • #4
yeah i figured them out and yeah missed it off, thx
 
  • #5


Hello,

Thank you for your questions. Let's start with the first one. The Lie bracket [u,v] represents the commutator of two vector fields u and v, and it is defined as [u,v] = u(v) - v(u), where u(v) denotes the action of u on v. In your proof, you have correctly shown that [u,v]w = \mathcal{L}_{[u,v]}w, where \mathcal{L}_{[u,v]} denotes the Lie derivative of w along the vector field [u,v]. This means that the two expressions are equivalent.

For your second question, the Lie bracket [X,Y] is not equivalent to the expression you have written. The Lie bracket is a vector field, while the expression you have written is a differential operator. To calculate [X,Y], you need to use the definition of the Lie bracket mentioned above. First, calculate X(Y) and Y(X), and then subtract Y(X) from X(Y) to get [X,Y]. I am not sure what you mean by expanding it further, but you can apply the same process to calculate higher order Lie brackets.

I hope this helps clarify your doubts. If you have any further questions, please feel free to ask.
 

FAQ: Are Lie Brackets and Their Derivatives Equivalent in Vector Field Calculations?

What is a Lie bracket?

A Lie bracket, also known as a commutator, is a mathematical operation that measures the failure of two operations to commute with each other. In other words, it measures how much the order in which two operations are performed affects the final result.

What is the relationship between Lie brackets and derivatives?

Lie brackets and derivatives are closely related in the field of differential geometry. In general, the Lie bracket of two vector fields corresponds to the derivative of the Lie group action associated with those vector fields. This means that the Lie bracket can be seen as a generalization of the derivative operation.

How are Lie brackets and derivatives calculated?

The calculation of a Lie bracket involves taking the commutator of two vector fields, which is done by taking the difference between the two vector fields and then substituting in the appropriate coordinates. Derivatives, on the other hand, are calculated by taking the limit of the difference quotient as the change in the independent variable approaches zero.

What are some applications of Lie brackets and derivatives?

Lie brackets and derivatives have many applications in mathematics and physics. They are used in the study of Lie groups, which are groups that are also smooth manifolds. They are also used in the theory of differential equations, as well as in mechanics and control theory.

What are some common properties of Lie brackets and derivatives?

One common property of Lie brackets and derivatives is that they both satisfy the Leibniz rule, which states that the derivative of a product is equal to the sum of the products of the derivatives. Additionally, both operations are linear and are related to the concept of tangency in differential geometry.

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