On top of the excellent comments of LostaEata, I would like to add my two cents on this topic.
Please forgive me in advance if my comments are too lengthy and boring.
According to AREMA 2006 Part 7 Existing Bridges and Part 9 Commentary, LF should be applied 8 ft above top of rail for Braking, and 3 ft for Traction. Section 15-9.1.3.12 says, “This force is transferred from vehicle to rail as a horizontal force at the top of rail and a vertical force couple transmitted through the wheels.”
It is fairly straight forward for the horizontal force applied at top of rail. However, it is not so clear for the vertical force couple. To understand the vertical force transfer into the bridge members, I would like to introduce two modeling concepts: (1) External Mass and (2) Internal Mass. The first model can be used for calculating forces at bearings and the second one will be useful in understanding how each structural member reacts to LF.
1. External Mass Model for Forces at Bearing
The external mass consists of a solid rectangular box rests on two simple supports. The rectangular solid box represents the entire superstructure as a whole. When LF is applied at 8 ft or 3 ft above the rail, this solid box directly transfers the load to the bearings creating a vertical force couple at the bearings. Some people may raise a question, “How can a force go up? Well, there are plenty of other downward loads such as Live Load and Dead Load to prevent one end from being lifted up. So, moment (M = LF x Arm) will be resisted by the vertical force couple: one goes up and the other goes down at the bearings.
The horizontal force will be transferred to the bearings also based on their fixed conditions. These horizontal force and vertical forces will be used to check the bearing materials as well as anchor bolts capacity and substructure members.
2. Internal Mass Model for Individual Structural Members
Unlike the external mass model, the superstructure is no longer a solid box in the internal mass model. It rather consists of many different structural members such as stringers, floorbeams, plate girders and truss members. In bridges with stringers and floorbeams, LF is first applied to the stringers and then must be transferred to the members to which stringers are connected, usually the floorbeams.
When modeling this internal mass in computer analysis software, it is recommended to apply LF at as many locations as possible rather than at only one location. If LF is applied at one location, the structural elements right underneath the application point will experience excessive stress. It is recommended to apply LF at the location of each floorbeam. For example, if the total LF is 200 kips and total number of floorbeams is 20, then 10 kips of horizontal force will be applied at each floorbeam location at the elevation of 8 ft above the rail top. For application arm linked to 8 ft for braking and 3 ft for traction, it is recommended to create weightless rigid member and apply LF on top of those dummy members.
When calculating the forces by hand, the floorbeams will get even horizontal force. When it comes to vertical force at floorbeams, it is recommended to use a group of pile analogy. Imagine there are 20 piles lined up in one row and then the moment created by LF x Arm will be resisted by this 20 piles. The outer piles will get more loads than the inner piles. The vertical pile reaction, p = M* xi / sum (xi ^2) from pile design.
I think that’s enough for today.
Thanks for your attention.