Solving Einstein Notation: Summing Subscripts and Superscripts

andrewkirk
Science Advisor
Homework Helper
Insights Author
Gold Member
Messages
4,140
Reaction score
1,741
\vec{v} = v^i\vec{e}_i = g(\vec{v},\vec{e}_i)\vec{e}_i

The last bit is a sum over i but will need a Ʃ because the Einstein rule only applies to matched superscripts and subscripts and here bot the i are subscripts.

Even if I write out the metric in the basis it doesn't work:

g(\vec{v},\vec{e}_i)\vec{e}_i=g_{ab}v^ae^{b}_{i} \vec{e}_i

In everything else I've ever done the indices have always been where they needed to be for Einstein summation but for some reason in this one they're not. It's no hardship to write the \Sigma^{n}_{i=1} before it but it just feels as though there should be a way to avoid that.

Any suggestions or comments? Thanks very much.
 
Physics news on Phys.org
You can use the dual basis, defined by

e^i (e_j) = \delta^i{}_j
Then you have

v = v^i e_i = e^i (v) \, e_i
 
Thanks very much. I thought there had to be a way.

\vec{v}=v^i\vec{e}_i=\tilde{e}^i(\vec{v})\vec{e}_i

Beautiful!
 
Thread 'Can this experiment break Lorentz symmetry?'
1. The Big Idea: According to Einstein’s relativity, all motion is relative. You can’t tell if you’re moving at a constant velocity without looking outside. But what if there is a universal “rest frame” (like the old idea of the “ether”)? This experiment tries to find out by looking for tiny, directional differences in how objects move inside a sealed box. 2. How It Works: The Two-Stage Process Imagine a perfectly isolated spacecraft (our lab) moving through space at some unknown speed V...
Insights auto threads is broken atm, so I'm manually creating these for new Insight articles. The Relativator was sold by (as printed) Atomic Laboratories, Inc. 3086 Claremont Ave, Berkeley 5, California , which seems to be a division of Cenco Instruments (Central Scientific Company)... Source: https://www.physicsforums.com/insights/relativator-circular-slide-rule-simulated-with-desmos/ by @robphy
Does the speed of light change in a gravitational field depending on whether the direction of travel is parallel to the field, or perpendicular to the field? And is it the same in both directions at each orientation? This question could be answered experimentally to some degree of accuracy. Experiment design: Place two identical clocks A and B on the circumference of a wheel at opposite ends of the diameter of length L. The wheel is positioned upright, i.e., perpendicular to the ground...
Back
Top