OK, this is me, "just asking a question".
I was wandering around in the ALSJ (I could get lost in there for days if I could find someone to bring me sandwiches) and I found a spot where Dave Scott, Apollo 15 CDR and first man to operate the LRV on the lunar surface, had some comments about the stability of the Rover and what it might take to cause a rollover. He and Eric Jones are talking about their (Scott and LMP James Irwin) return from Geo Station 2, driving downhill from Hadley Delta when the front wheels dug in and sent them into a sudden 180o spin.
[Jones - "You remember the 180? Which way did the back end go?"]
[Scott - "I think to the right. I don't really recall, but I remember it was real quick, before you could do anything about it. As I said here, the front wheels dig in. We were trying to maneuver around stuff, and it just broke. It was over before we even knew it. That's why we're laughing. Tsuuuu! and around it went. And then we went uphill, turned around, and came back downhill. And I know that the people in the back row at the Control Center were probably all crossing their legs tight."]
[Jones - "And it was basically a really stable little vehicle."]
[Scott - "Very stable. There was never any feeling of maybe turning over, at all. That's why it (incidents like the 180) was interesting: even though the rear end broke out - several times - and you spin all the way around, you don't have any feeling that it's going to turn over. It's sliding"]
[Jones - "Gene said that on their third EVA, when they were doing a fair bit of cross-slope driving on the North Massif, they had the feeling that if the upslope wheels started bouncing that they were getting toward the margins of stability. Did you ever have that feeling?"]
[Scott - "Nope. Gee, it's hard to imagine. I think you'd have to go look at the c.g. (center-of-gravity) and it would be easy to calculate. 'Cause if you know the c.g. and you know the angle the Rover is driving, you know the difference between the center of gravity and the center of pressure and you can figure our how much force it would take to push it over. And I think'd be really difficult to turn over."]
[Jones - "You'd have to be well tilted and you'd really have to bounce the uphill wheels."]
[Scott - "And you don't get a lot of angular momentum from the force, because of the low g. It's just kinematics, freshman physics."]
[Jones - "Assume you're going along at some tilt angle and at some speed and you hit a crater which gives you a force."]
[Scott - "And your force would be a reactive force from the Rover, which is limited by the Rover mass. There's nobody pushing you, so it has to be a wheel going into a crater to create a reactive force. Boy, I think it would be hard to get enough reactive force, with the suspension system which damps out the force. Boy, tough to do, but it could probably be done. It'd be interesting. If you were going very fast, then you've got a lot of energy in the system and, you might translate the energy into an overturning moment. It would be a great little exercise for somebody at school."]
Would someone be so kind as to clarify the part of the conversation I've marked in red, especially the underlined sentence? I get the general principles, but I'm not clear on what is meant by "reactive force" in this context and how it relates to the mass of the rover.
Thanks.