whatif said:
Thank you. I understood that it is in the timelike direction. My difficulty is interpreting what that physically means, especially coming from thinking that energy is a scalar quantity. I do not have the same problem with momentum.
If you understand spatial basis vectors, then specifying three spatial basis vectors, for instance the spatial basis vectors of an observer "at rest" in some coordinate system in the Minkowskii space of special relativity, uniquely define one time-like vector that is orthogonal to all three spatial vectors.
Hopefully the notion of orthogonality is familiar. Formally, two vectors are orthogonal if their dot-product is zero. And hopefully the notion of the dot-product of four-vectors is familiar. If not, I would guess a review is in order, I'm not sure how to explain things further without using these concepts.
A note on terminology here, to avoid confusion. We usually say "space-like" vectors as an adjective when we talk about four-vectors rather than "spatial" vectors. Then a "purely spatial" four-vector would be a four-vector with no component in the time "direction".
The mathemtics then are that specifying three space-like vectors mathematically defines a unique time-like vector that's orthogonal to all of the space-like vectors. Similarly, if we define a time-like vector, we can determine three space-like vectors that are orthogonal to the time-like vector, and to each other. However, this set of space-like vectors with this property is not unique because of the existence of spatial rotations. Performing purely spatial rotations of the three space-like vectors will generate a different set of space-like vectors that meet our orthogonality conditions.
Thus specifying a set of three space-like vectors automatically specifies a time-like vector that's orthognal to all of them.
You hopefully recall that simultaneity is relative in special relativity. If not, you need to study the issue, it's important. The fact that different observers, those moving with different velocity, have different notions of simultaneity is closely related to the fact that the time-like four-vectors that are associated with these observers are different vectors. The name of the time-like four-vector associated with an observer may also be useful, it's called the observers four-velocity vector.
Making a vectors purely spatial basically implies that we set the time-component of the vectors to zero if we assuming Minkowskii coordinate conventions. As a consequence of defining what it means for a vector to have no time component, we have implicitly defined the notion of what a time-component is, and how to set that time component to zero. This specifies a notion of simultaneity, and the notion of simultaneity depends on the observer, in particular the state of motion of the observer.
Mathematically, the notion of dot-product comes first, and we use the notion of dot-product of an arbitrary vector with a basis vector to define the meaning of a component of a vector. A components of an arbitrary vector, accordign to the mathematical defintion, is the dot product of the arbitrary vector with the basis vector.
Your intuition is probably working backwards from the formal mathematical definition, assigning physical significance to the "vanishing" of the time component. This is exactly backwards from the mathematical approach, which treats vectors as abstract entities with abstract properties, and the "frame of reference" of an observer is a physical interpretation of the mathematical representation of a set of mutually orthogonal basis vectors associated with the observer.
The relativity of simlultaneity means that the notion of making the "time-component" of a vector "vanish" depends on the choice of basis vectors used. The mathematical description starts with the basis vectors, and allows one to define an observer as a set of basis vectors. The intuitive notion usually goes backwards, one defines an "observer" intuitively first, then finds set of basis vectors associated with that observer.