Outer space: Rowing has its moments
If you look at the pattern of rowers in a racing four or eight rowing boat then you expect to find them positioned in a symmetrical fashion, alternately right-left, right-left as you go from one end of the boat of the boat to the other. This pattern is called the rig of the boat and the conventional one we have just described is called the standard rig, shown here for a Four
and an Eight.
The standard rig for a rowing Four and Eight.
However, the regularity of the rower's positions hides a significant asymmetry that affects the way the boat will move through the water. Some time ago I looked at the rig of racing boats in a different way. Recall that in a rowing boat the rowers sit facing backward, so it is when they pull the oar towards them that the boat is propelled through the water. The pulling motion exerts a force on
the boat in the direction of its forward motion. But since the end of the oar held by the rower describes a circular arc, there is also a second component to the total force acting on the boat at the rowlock. Its direction is at right angles to the boat's forward motion. During the first half of the stroke it is directed towards the boat but during the second recovery phase the force is
in the opposite direction, at right angles to the boat but away from it. As a result the boat is subject to a sideways force that alternates, first towards the boat, then away from it.
On the first part of the stroke (top) the transverse force acts towards the boat and on the second part (bottom) it acts away from the boat.
If we go to the back of the boat we can take moments (measuring the turning effect) of these sideways forces. Each is equal to the magnitude of the force times the distance to the point of application of the force. For simplicity, let’s assume the rowers have identical strengths, equal to "vertical-align:0px; width:13px; height:12px" class="math gen" />, the first rower (the stroke) is at a distance from the end of the boat and all the other rowers are equally spaced, a distance apart. During the first half stroke the sum of the moments of the transverse forces acting on the four rowers in a Four is
(The transverse force acts in opposing directions for rowers on opposite sides of the boat, hence the alternating sign of in this equation.)
Notice that the answer is not zero! Also, conveniently, the distance to the first rower, , just cancels out because there are the same number of rowers on each side of the boat (the boat would go around in circles otherwise!). In the second phases
of the stroke everything is the same except that the direction of the force reverses. This simply means changing "math gen" /> to in our formula. So, as the boat is propelled forwards it is subjected to an alternating sideways force that varies between "vertical-align:-2px; width:41px; height:14px" class="math gen" /> and : the boat wiggles.
If there is no cox the rowers have to sense this wiggle and expend energy cancelling it out by counter sideways movements. If there is a cox then he or she will use the rudder to counter the wiggle. Both actions use up energy that could otherwise be propelling the boat forwards.
We can avoid the wiggle by repositioning the rowers. In the case of the Four, a rig that goes right-left-left-right, as shown below results in no net sideways moment on the boat because we have
The zero moment Four rig.
This seating plan is known as the Italian rig because it was discovered by the Moto Guzzi Club team on Lake Como in 1956. The crew of the Club's Four was being watched by Giulio Cesare Carcano, one of the company's leading motorcycle engineers from Milan, who suggested that the failure of the boat to run straight might be alleviated by putting the middle two oarsmen both on the
starboard side with the stroke and the bow still on the port side. The result was rather successful and the Moto Guzzi crew went on to represent Italy and take the gold medal that year at the Melbourne Olympic Games.
The situation for an Eight is more complicated. The standard rig produces a non-zero sideways moment that alternates between and "vertical-align:-2px; width:41px; height:14px" class="math gen" /> during each stroke. The cox is going to have to work hard to counter that wiggle. But I found that there are only four possible ways that an Eight, crewed by identical rowers, can have a zero sideways moment. Here are the four no-wiggle rigs:
The four possible rigs for Eights which have zero transverse moment. (a) The new rig 1: uudddduu; (b) The German rig: ududdudu; (c) The Italian rig: udduuddu; and (d) The new rig 2: udduduud.
Rig (c) is just two of the Italian rigs for a Four set one behind the other. Rig (b) is the so called German, bucket, or Ratzeburg rig, first used by crews training at the famous German Ratzeburg rowing club in the late 1950s under Karl Adam, who was motivated by Carcano's configuration for the Four.
The other two rigs are new.
When I published these results they attracted a lot of attention around the world and there were articles about them in World Rowing Magazine. The results were then confirmed in greater detail in an article in the
Rowing Biomechanics Newsletter. New Scientist magazine then prepared a long article about them and commissioned some trials on the River Thames with the Imperial College Eight (see the picture below) to see how they liked the new rig (a) compared to the standard one. Then I discovered that the winning Canadian Men's Eight used the German rig (b) in their gold medal race at the
Beijing Olympics and Oxford did the same to win the 2011 University Boat Race on the Thames – the first time a non-standard rig had been used in the race for 40 years. However, the reason was one of convenience in fitting in some outsized oarsmen rather than the desire to be wiggle-free. Perhaps someone will try my (a) or (d) in London 2012.
A trial of one of the new rigs on the Thames, organised by New Scientist. Image copyright Mark Chilvers.
You can watch a New Scientist video exploring John Barrow's ideas for efficient rowing rigs on YouTube.