In addition, the problem of the 6:00 o'clock thin section of the barrel shank only became a problem when the 125 grain/1,400 fps loads hit LE holsters.
No one that I know of who used 158 grain magnums ever had trouble.
That makes sense as the issue is the tiny fraction of a second dwell time that it takes for the entire length of the bullet to clear the barrel/cylinder gap.
Apparently, the shorter length of the 125 grain and under bullet weights left the barrel/cylinder gap unsealed by the bullet itself for just enough time less than the longer bullets that the temperature of the flame was just too much.
That is the reason that the FBI and others went to bullets of no less than 140 grains. The extra length kept the barrel/cylinder gap sealed just that tiny fraction of a second longer so as to make the flame cutting and ultimate damage not a problem.
Continuous use of magnums in the K frame was just not an issue for anyone who stayed with 140 and above. Of course, by the time it was figured out, guns were destroyed, and some people never got the message.
When Bill Jordan proposed the idea of the K frame magnum, it was thought that magnums (158 grains) would be used for carry and qualification only. All other practice would be with 38 target wadcutters.
So, it took a combination of all practice with magnums and the 125 grain at 1,400 fps to cause the issue.
I like the post, except for the bold bit.
From a thermodynamics perspective, the small amount of plasma that might beat the bullet to the forcing cone doesn't have enough time to act on the the forcing cone and heat it to any significant degree. The short bullet explanation sounds great on the surface, but it just doesn't hold up when you apply some science to it.
Additional heat however is the issue. Let's look at Hornady XTP data for different bullet weights using Hodgdon H-110/Win 296, and Alliant 2400.
Maximum loads of H-110 (a colloidal ball powder):
- 180 gr XTP, 13.1 grains
- 158 gr XTP, 15.6 grains
- 140 gr XTP, 18.4 grains
- 125 gr XTP, 19.9 grains
In this case, the 125 gr load has 28% more powder than the 158 gr load.
Maximum loads of 2400 (a flattened spherical powder)
- 180 gr XTP, 12.6 grains
- 158 gr XTP, 14.3 grains
- 140 gr XTP, 15.5 grains
- 125 gr XTP, 16.9 grains
- 110 gr XTP, 18.8 grains
In this case, the 125 gr load has just 18% more powder than the 158 gr load.
The point here is that the hot loads with 125 gr bullets have significantly more slow burning powder that flows through the forcing cone in a partially burnt and abrasive state along with a larger amount of hot plasma and with significantly more heat.
The increased heat from the larger powder charge, applied to the forcing cone, along with the larger amount of partially burnt powder flowing through the forcing cone with that plasma produces significantly more erosion of the forcing cone.
That erosion creates "v" shaped cuts in the forcing cone and those V shaped cuts are stress risers. Since the forcing cone is thinner where it has been milled flat, that area is more susceptible to cracking.
In short, it's not the shorter bullet, but rather a combination of 1) a larger charge of a 2) slower burning colloidal ball powder, used with the lighter weight bullet.
If you look at the data above, you'll also note the absence of an H-110 charge for a 110 grain bullet. Those slow burning colloidal ball powders are not efficient with a 110 gr bullet, and despite it's even shorter length, you don't hear about cracked forcing cones due to 110 grain loads.