The box pulling on the wire applies a tension to the wire. Tension is a force, measured in Newtons. If we make some simplifying assumptions (no friction between wire and environment) then the tension is the same at all points along the wire.

If we consider your example to be static, then the tension on the wire is just the weight of the box:

T = m * g

where m is the mass of the box and g is acceleration due to gravity (i.e. 9.8 m/s^2). Note this is only valid in the static case, see below for an explanation of how to calculate it in the dynamic case.

The force at each bend in the wire is then just the projection of the tension onto the relevant direction. For example the force at the tip of the spring object is a downward force of magnitude:

F = T * cos(angle between wire and spring axis)

The force at your second marked point on the environment is irrelevant, since it has no impact on the tension or anything else.

Now, in the dynamic case the tension is simply the constraint force which you apply to the box in order to keep it attached to the wire. So if the physics engine is impulse based, the tension is just:

T = impulse / timestep

This leads into the general algorithm for wrapping the wire around the environment too. The important property is the total length of the wire. Only the last segment needs to be simulated, all the earlier segments can be considered to be fixed. So the length of the last segment is known, just subtract the lengths of the earlier segments from the total length. Then the last segment can be a simple spring constraint. Then just split a segment whenever it intersects with the environment, and remove the split when the bend straightens out.

The box pulling on the wire applies a tension to the wire. Tension is a force, measured in Newtons. If we make some simplifying assumptions (no friction between wire and environment) then the tension is the same at all points along the wire.

If we consider your example to be static, then the tension on the wire is just the weight of the box:

T = m * g

where m is the mass of the box and g is acceleration due to gravity (i.e. 9.8 m/s^2). Note this is only valid in the static case, see below for an explanation of how to calculate it in the dynamic case.

The force at each bend in the wire is then just the projection of the tension onto the relevant direction. For example the force at the tip of the spring object is a force along the contact normal, of magnitude:

F = T * cos(angle between wire and contact normal)

In this case the contact normal direction would be the bisection of the angle between the wire segments. The force at your second marked point on the environment is irrelevant, since it has no impact on the tension or anything else.

Now, in the dynamic case the tension is simply the constraint force which you apply to the box in order to keep it attached to the wire. So if the physics engine is impulse based, the tension is just:

T = impulse / timestep

This leads into the general algorithm for wrapping the wire around the environment too. The important property is the total length of the wire. Only the last segment needs to be simulated, all the earlier segments can be considered to be fixed. So the length of the last segment is known, just subtract the lengths of the earlier segments from the total length. Then the last segment can be a simple spring constraint. Then just split a segment whenever it intersects with the environment, and remove the split when the bend straightens out.