Mahanakorn's Physics Magic: The Wall Of Death
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Quick explanation (fuller explanation further down below):
"The gravity force downwards is balanced by the friction force upwards, with the normal reaction from the wall providing both the force needed for circular motion and the complex restoring torque needed for balance."
A. THE DANGERS:
The frictional force needs to be high enough on the wall ( so don't try it with wet walls )
Vehicle speed needs to stay above a calculable minimum ( so don't go too slowly! )
Motorcycles must lean at a speed dependent angle to prevent tipping over: the higher the speed, the smaller the needed lean angle.
Cars cannot lean but they do not need to (see why below).
Riders in cars on the wall should lean to reduce nausea and muscle strain.
B. THE PHYSICS CONCEPTS:
 the maximum static frictional force (F_{F}) is proportional to the normal reaction (N), where the normal reaction is the always observed perpendicular push back by a surface when it receives a force
 the force causing motion in a circle acts towards the centre of the circle and can be written as F_{c}= mv^{2}/r, where m and v are the mass and velocity of the rotating body and r is the radius of the rotation;
 the force (down) due to gravitational attraction can be written F = mg;
 the centre of mass of a body is the point that, if all the mass were concentrated there, would behave translationally just like the real body does;
 if force is applied to a body at a distance from a pivot point, then the body will tend to rotate about that pivot point, with the size of the rotation determined by multiplying the force by the perpendicular distance (the answer being a number we call "torque");
 any force which does not act along a line through the centre of mass will produce a torque (and hence a tendency to rotate);
 precession (like that seen in a spinning top) needs a torque applied to stop it.
C. THE PHYSICS DETAILS:
For a body of mass m moving in a horizontal circle on a wall of death, the normal reaction from the wall is what supplies the force necessary to obtain motion in a circle.
So we can write: N = mv^{2}/r
If the body does not slide down the wall, then the pull of gravity downwards must be balanced by the frictional force (due to the ‘roughness' of the wall) upwards.
So the force diagram looks like:
This frictional force can vary as needed up to a maximum of .
But how much frictional force is available depends on the speed, which means there will be a MINIMUM speed for revolution at a constant height above the ground. This minimum speed will be the one for which the maximum frictional force exactly equals the gravitational pull on the mass (since any lower frictional force will not be strong enough to provide the balance).
Higher speeds will also produce no slipping, but as the speed rises steering and control will become more difficult.
So when , then v is the lowest it can be (ie v_{MINIMUM} ), for no slipping to occur. Which means the minimum safe speed is .
BUT:
The above analysis assumes a point mass (i.e. with all the mass concentrated in a single point located at the centre of mass and all the forces acting on that point).
However for a motorcycle on the wall of death, although the weight acts through the centre of mass, the friction acts at the wheels (on the wall).
These three forces (friction forces on each of the tyres, a weight force through the centre of mass) balance but are not in the same line. Which means the motorcycle will tend to rotate and tip over.
The normal reactions from the wall (acting where the tyres touch the wall) cannot help to balance this torque because they will not produce any turning effect if the motorcycle is perpendicular to the wall:
But if the motorcycle leans at an angle to the vertical to the wall then the normal reactions from the wall, will produce a tendency to rotate (a torque) in the opposite direction.
So if the rider leans the motorcycle at the correct angle then the torques will be equal and no rotation will occur.
For other angles of lean there will be unbalanced torques causing the motorcycle to rotate and fall.
At these other angles of lean the rider's muscles will need to push more strongly in order to supply the extra torque to maintain balance. The rider may also experience nausea (because the endolymph fluid in the ear will experience an unbalanced torque and rotate).
Note that precise reasoning is more complicated than this since different parts of the motorcyclerider system are at different distances from the cylinder axis and so there is a need to consider the effect of the torque on the nonzero angular momentum which gives rise to precession of the rider and bike about the centre of mass (for all angles except the "correct" one)! For discussion of this complex issue see J. McCullen and L. McIntyre, The Physics Teacher , 36, 389 (October, 1998).
With cars however the precession can't occur. Cars do not need to lean as long as they have a relatively wide wheelbase and a low centre of mass. To see why read the analysis below.
WHY DO CARS NOT NEED TO LEAN?
Summary : When a car is running around a vertical wall, the tyres closer to the ground experience stronger normal reaction force than the tyres opposite them (closer to the top of the wall). So, provided the speed is high enough, the counterclockwise torque from the normal reaction of the lower tyres can provide the extra balancing torque without the need to lean. Details: Consider the diagram below showing the relevant forces and distances.
Define:
N_{upper} (lower) = sum of the normal reactions of the upper ( lower ) front and rear wheels;
F_{upper} (lower) = sum of the friction forces of the upper ( lower ) front and rear wheels;
L = the wheelbase (distance between the front or back wheels, assumed the same)
H = perpendicular distance from the car's centre of mass to the Wall;
v = speed of the centre of mass of the car;
R = radius of the circular path travelled by the centre of mass of the car;
= static friction coefficient between the Wall and the tyres.
Assume the centre of mass of the car to be on the plane that perpendicularly bisects the wheelbase.
Force analysis reveals:
(i) total normal reaction from the Wall provides the circular motion force (F_{c}):
...............................N_{upper} + N_{lower} = F_{c}= mv^{2}/r .........................................…… (A)
(ii) total frictional force balances the weight:
...............................F_{upper} + F _{lower} = mg ......................................................…… (B)
Torques (about the car's centre of mass) yield:
...............................(N_{ upper})(L/2) + (F_{upper} + F_{lower} )(H) = (N_{lower} )(L/2).................... ......(C)
Hence:
...............................N_{upper }= (1/2) (mv^{2}/r) – (H/L)(mg) F_{lower} = (1/2) (mv^{2}/r) + (H/L)(mg)
Since F_{upper} can never be negative (because walls can only push, never pull), then:
(i) ..............{"no flip"}
For safety, at maximum friction , (N_{upper} + N_{lower} ) > mg, so:
(ii) ................{"no slip"}
Both conditions must apply simultaneously  meaning the minimum nolean speed required for travel on a Wall of death of given radius is determined by whichever is the greater of (1/ ) and (2H/L).
For bodies with a wide wheelbase and a low positioned centre of mass (say, standard cars), the ratio 2H/L will be small, so the reciprocal of the friction coefficient becomes the most important factor (i.e. do it on dry days only!) and the minimum nolean speed is easily attainable.
For bodies with a short wheelbase and a high positioned centre of mass (say, rollerblade riders), the ratio 2H/L will be large so the minimum nolean speed becomes impracticably high. A motorcycle would be the limiting case of this, since L is effectively zero and hence no nolean speed possible.
Which is what we found when riding our real Wall of Death: cars do not lean, motorcycles do!
