zanick said:
Why wouldn't the higher tangential velocity at take off and therefore , greater linear momentum vs that plane a destination on the same longitude, aid in getting to the destination ?
The surface of the Earth is an equipotential surface in the rotating frame.
Edit to add...
An equipotential surface is [obviously] a surface along which potential energy is a constant. Conservation of energy allows you to conclude that an object freely following the surface retains constant kinetic energy and, accordingly, constant speed.
In the case of the surface of a rotating Earth, there are two contributions to the potential: Gravitational force and centrifugal force. Both have associated potential fields. We are all familiar with the gravitational potential field. It scales as the inverse of the radius [from the center of a spherically symmetric gravitating object as long as one is in the region outside said object].
We are not often taught about the potential field associated with the centrifugal force. However, it has one. It is, after all, a central force whose magnitude depends only on the distance from the center. It follows that it has a potential field. The force scales as the square of distance from the center. The potential (the integral of the force), accordingly, scales with the cube of the distance from the center.
If you take the sum of the gravitational potential and the centrifugal potential and find the set of points where that sum takes on a particular value, you have an equipotential surface. Along this surface, the vector sum of centrifugal force and gravitational force always points tangent to the surface.
An object that is rolling, flying or otherwise moving along this equipotential surface never experiences any forward, rearward or side-ward acceleration due to the vector sum of centrifugal and gravitational force. The vector sum of the two forces (i.e. a plumb line) is always normal to the surface.
What about Coriolis force, you may ask. The answer is that Coriolis can produce a sideways force. But a sideways force never alters an object's velocity. As judged from the rotating frame,
the Coriolis force can never do work. It can never make an object move faster or more slowly. It can only change an object's direction of motion.
Billiard balls do not roll northeast more easily than southwest.
Edit again...
The above is an analysis in the rotating frame. If you are going to speak of the Coriolis force at all, you need to jump in with both feet and adopt the rotating frame. It is no fair cheating and mixing in references to effects that hold in the inertial frame. That'll just get you labelled as a "frame jumper" and all the kids on the playground will start laughing behind your back.
If you try to analyze the situation from the inertial frame you have a problem: You are not flying north-east any more. Nor are you trying to reach a point north-east of where you started. You are jumping off from a moving point and trying to intercept another moving point while swimming in a moving fluid. [The complexity of this problem is what motivates the shift to the rotating frame of reference]
Attaining a high eastward velocity is no longer an important metric for success. Instead, you'll need a westward acceleration to match speeds with your destination. That "Coriolis" boost that you were expecting to help you is actually a velocity delta that you eventually need to fight.