Tensor equation in Dirac's 1975 book

In summary, the Dirac equation, which is represented by x^{\lambda}_{,\mu}x^{\mu}_{,\nu}=g^{\lambda}_{\nu}, does not have a 4 on the right side. When expanded, the equation shows that the first term, for example, is 1 and all off-diagonal terms are 0. This is consistent with the special case of the identity transformation.
  • #1
exmarine
241
11
Dirac has equation 3.4 as:

x[itex]^{\lambda}_{,\mu}[/itex]x[itex]^{\mu}_{,\nu}[/itex]=g[itex]^{\lambda}_{\nu}[/itex]

Shouldn't that have a 4 on the right side?

x[itex]^{\lambda}_{,\mu}[/itex]x[itex]^{\mu}_{,\nu}[/itex]=(4?)g[itex]^{\lambda}_{\nu}[/itex]
 
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  • #2
exmarine said:
Dirac has equation 3.4 as:

x[itex]^{\lambda}_{,\mu}[/itex]x[itex]^{\mu}_{,\nu}[/itex]=g[itex]^{\lambda}_{\nu}[/itex]

Shouldn't that have a 4 on the right side?

x[itex]^{\lambda}_{,\mu}[/itex]x[itex]^{\mu}_{,\nu}[/itex]=(4?)g[itex]^{\lambda}_{\nu}[/itex]

Nope. let me open the expression for you


[itex]\Sigma _ \mu \frac{\partial x^ \lambda}{\partial x ^ \mu} \frac{\partial x^ \mu}{\partial x ^ \nu}=\delta ^ \lambda _ \nu = g ^ \lambda _ \nu [/itex]
 
  • #3
Let me open it some more

[itex]
\Sigma _ \mu \frac{\partial x^ \lambda}{\partial x ^ \mu} \frac{\partial x^ \mu}{\partial x ^ \nu}=\Sigma _ \mu \delta ^ \lambda _ \mu \delta ^ \mu _ \nu =\delta ^ \lambda _ \nu = g ^ \lambda _ \nu [/itex]
 
  • #4
? Wouldn't the first term, for example, be:

[itex]\frac{\partial x^{0}}{\partial x^{0'}}[/itex][itex]\frac{\partial x^{0'}}{\partial x^{0}}[/itex]+[itex]\frac{\partial x^{0}}{\partial x^{1'}}[/itex][itex]\frac{\partial x^{1'}}{\partial x^{0}}[/itex]+[itex]\frac{\partial x^{0}}{\partial x^{2'}}[/itex][itex]\frac{\partial x^{2'}}{\partial x^{0}}[/itex]+[itex]\frac{\partial x^{0}}{\partial x^{3'}}[/itex][itex]\frac{\partial x^{3'}}{\partial x^{0}}[/itex]=4?

And all the off-diagonals be 0 of course.
 
  • #5
Consider the special case of the identity transformation, where all the new coordinates are the same as the old ones. That is, x0' = x0, x1' = x1, x2' = x2, and x3' = x3. Plug this into your equation, and I think you'll see that the result is 1, not 4.
 

Related to Tensor equation in Dirac's 1975 book

1. What is a tensor equation?

A tensor equation is a mathematical equation that describes the relationship between tensor quantities. Tensors are mathematical objects that represent physical quantities and their transformations in different coordinate systems. In physics, tensor equations are commonly used to describe the behavior of physical systems, such as the laws of motion in classical mechanics or the equations of general relativity.

2. Who is Dirac and what is his 1975 book?

Paul Dirac was a British theoretical physicist who made significant contributions to the development of quantum mechanics and quantum field theory. His 1975 book, General Theory of Relativity, is a comprehensive textbook that presents a mathematical framework for understanding Einstein's theory of general relativity.

3. What is the significance of tensor equations in Dirac's 1975 book?

In his book, Dirac uses tensor equations extensively to describe the concepts and principles of general relativity. This is because tensors are essential mathematical tools for understanding the geometry of curved spacetime, which is central to Einstein's theory. By using tensor equations, Dirac is able to show how gravitational interactions can be described in terms of the curvature of spacetime.

4. Are tensor equations difficult to understand?

Tensor equations can be challenging to grasp for those who are not familiar with advanced mathematics. They require a solid understanding of linear algebra and differential geometry. However, with the right background knowledge and practice, tensor equations can be understood and applied to solve complex physical problems.

5. How are tensor equations used in modern physics?

Tensor equations are used in various areas of modern physics, such as relativity, quantum mechanics, and electromagnetism. They provide a powerful mathematical framework for describing the behavior of physical systems and making predictions about their behavior. In addition, tensor equations are also used in the development of new theories and models in physics, such as string theory and loop quantum gravity.

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