The diameter of these pins must be given to determine the cross sectional area and the resulting shear stresses in the pins.
Analysis of this concept must also take into account the shear forces acting on the pins that hold the disks in place. If these forces are too great within the operating torque limits, then the pins will shear before the torque limiter even begins to compensate for any overloaded condition.
Shear Stress Analysis
And the spring constant is:
Therefore the required spring force to keep the disk at an angle during normal operation is:
The spring constant can then be found by
specifying the length that the spring must travel:
In equilibrium the Moment equation is equal to 0, therefore we can solve for the spring force.
Therefore it appears that a material may be chosen for the pins to withstand the shear
stresses involved.
And the Tensile yield Strength is:
For Type 301 cold rolled stainless steel:
In this case, this steel would not be suitable for the pins
However the Tensile yield Strength is:
For 1040 hot rolled steel The ultimate tensile strength is :
Depending on the material chosen for the pins, this design may or may not hold up to the required torque levels.
The shear force on the pins will depend on the angle of the disk and the Force from the maximum allowable torque of the shaft:
Given an angle of the disk with respect to the axis perpendicular to the axis of rotation of the shaft:
The geometry of the design will place a normal force on the second disk as a result of the force from the torque. Based on the angle of the disk this component of the force can be found. The reaction force from the second disc is equal to this force when the system is in equilibrium.
The Force located at this point on the
shaft can be calculated using the equation:
A tangential force will result on the end of the shaft
dependant on the radius of the point in question

For a given radius:
With a given torque limit:
Spring Force Analysis
Seizure Recovery System for Fuel System Distributor
Concept #4
The distance from the point of contact of the spring to the pivoting axis of disk 1 must also be specified. However this distance will change as the disk is tilted. Using the distance between these two points when the disk is in a vertical position, this length can be calculated for any angle:
The distance of the force acting on disk one from the pivoting axis of the disk
is found from the equation:
But first the distances d2 and d1 must be calculated
The width of the disks must be specified to find the
distance between the two pivoting axes of the disks
By analyzing the moment about the pivoting
axis of disk 1 we can solve for this spring force:

:
During normal operation this normal force is balanced by
a force from the spring in a direction that directly opposes it.
The normal force acting on the
disk from the spring is determined by: