We’ve had discussions about the F6F stall speeds in the past. Numbers from different sources vary. A snapshot from the Joint Fighter Conference in 1944 is interesting. At the conference flight tests for the stall speeds of the F6F-5 were (in knots):
F6f-5 (flown by11 Army, 2 British, 4 Navy, 10 Contractors)
Power off, clean: 65-81, 77 average
Power on, clean: 60-79, 69 average
Power off landing configuration: 55-75, 66 average
Power on landing configuration: 60-70, 65 average
Accelerated 3g: 105-150, 121 average
A couple of points can be drawn from this. First the variability in real life you can have in flight tests for the same plane. (I can’t remember if the F6F-5 was the exact same plane flown by every test pilot. It was at least the same configuration I believe.) Numerous real life factors play a part. In general comparing data from different flight tests can be problematic because the numbers tend to rarely line up exactly.
Second one of the causes of variability that effect stall speed is testing technique. Once upon a time we had a BBS discussion on this and how stall testing technique will result in different numbers in real life as well as in AH. I believe a key factor that could account for the lower stall speed numbers referenced in the film is due to the F6F’s nose attitude above horizon. In the film they demonstrated various stalls of the F6F. Here is a frame from the film just before the F6F enters a power-on stall in clean configuration.

In the picture notice the nose angle (attitude) above the horizon labeled as gamma. My rough guess is that’s a ~30 degree angle for gamma in the video. This angle can greatly impact stall speed results. Why? Because it changes the amount of weight, thus lift that wings must support. Here is a free body diagram that demonstrates this.

Notice that Lift = Weight * cosine ( gamma)
At level flight gamma=0, thus Lift=Weight since cosine(0)=1. However as nose angle (gamma) increases the amount of weight that lift must equal reduces based on the vector geometry. The greater the angle, the lower the stall speed will be because the airplane doesn’t have to produce as much lift to keep the airplane flying. In other words since lift is a function of lift coefficient and airspeed a plane can fly at Clmax at a lower velocity because the amount of lift needed to maintain flight is lower due to increased gamma.
Pyro posted some stall tests of the F4U that demonstrates this in action. The following are snapshots of power-off stalls where nose angle gamma was varied. The F4U was loaded at 12,904 lbs
Power off stall gamma = 7 degrees, weight=12,904 lbs.


Just before stall notice that the lift is 12,063 lbs, almost 850 lbs less than the 12,904lbs of weight. Stall speed is just about 103 mph.
Power-off stall at gamma=20 degrees, weight=12,904 lbs.


Just before stall lift=10,465 lbs, a full 2439 lbs less than the full weight. Stall speed is 98 mph.
The point here is that for the same airplane 1g stall speed varies depending on the amount of angle gamma above the horizon. In our example at 22 degrees stall speed is 98 mph vs. 7 degrees at 103 mph, a difference of 5 mph.To conclude, one of the factors that could play a noticeable factor in variations of stall speeds for the F6F in question is the technique used to test stall speed, specifically the angle of the nose above the horizon (gamma).
Tango