The Canoe Race

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The Canoe Race

The Canoe Race

A group of canoeists on holiday at the seaside decide to have a race offshore. They set up a triangular course using a buoy and two other floats, with the start and finish at the buoy. They have been told that the prevailing current flows parallel to the shore at a speed of about 2 ms-1. If the total course is to be 300 metres long investigate where they might place the other two floats.

Problem: How does the layout of the floats effect the time taken to complete the race?

I would like to investigate two different models one being a right-angled triangle and the other being isosceles triangle. When investigating the isosceles triangle, an equilateral triangle would be investigated because as the length of the isosceles triangle will all equal, it becomes an equilateral triangle. I would first of all investigate the right-angled triangle.

Model 1: Right-Angled Triangle

C

A B

PREVAILLING CURRENT AT A SPEED OF 2 MS-1

COASTLINE

Figure 1: The shape of the course (model 1).

The shape of the course is shown in figure 1. To simplify the problem I am assuming that the angle CAB is a right angle. Even though the lengths of B and C will change, angle CAB will always be a right angle. ‘A’ in figure 1is where the buoy is positioned, and thus it is the start and finish of the race. The race starts at point A, then it continues on to point B, then to point C and finishes at the buoy, which is point A. Point B and C are two floats, first and second float respectively. I will refer to the lengths AB, BC and AC, throughout the investigation.

It is more applicable to make assumptions; this would make the problem simpler. I will use the same assumptions for both the models. It is vital that we assume that the canoe is a particle and that it’s mass is concentrated at a single point. I will assume that there are no obstacles that may overcome the canoeists to alter their speed and direction. In a like manner they will not also bump into any object or each other. If these factors were taken into account, it would complicate the matter because these factors will slow down the speed or velocity of the canoeists. This will complicate the velocity diagrams. In reality the prevailing current will fluctuate in both magnitude and direction. To simplify the scale drawings, which I would use to solve the problems, there would not be any environmental factors, e.g. weather, which would affect the speed or velocity of the canoeists. Apart from the prevailing current, which flows parallel to the shore at a speed of 2ms-1, there are no other currents, no driving rain, no huge waves and no winds. The current has to have a direction, therefore, the prevailing current flows parallel to the shore at a speed of about 2 ms-1from left to right.

The total course will be 300metres. Hence AB + BC + CA = 300. When canoeing the canoe travels extra distance when climbing and descending waves, the extra distance will not be taken into account. The shape of the triangle or the course will have to remain the same or otherwise the canoeists will not travel the same distance. Therefore the shape and the positioning of the course will have to remain the same. If the course changed it will effect the time taken to complete the course. Thus, it will also presumed that the floats and the buoy are stable, therefore, they do not move with the current.

A sensible value for the speed of the canoeists would be 4ms-1 in motionless water. Furthermore, all the canoeists maintain both the same speed and direction; they will not be exhausted at any point of the race. Therefore, it will be taken into account that the canoeists will turn around a float at 4 ms-1 instantaneously, so that no extra time is taken in slowing down and turning the canoe at the floats. Therefore, the speed of the canoeists is constant. Furthermore, they travel in a straight line along the lengths AB, BC and CA in figure 1, so that no extra distance is travelled.

I will vary the length of AB in figure 1 in steps of 10 metres, i.e. 10, 20, 30, 40, 50, 60, 70, 80, 90, 100, 110, 120, 130 and 140. The length of AB in figure 1 cannot be or more than 150m. When each side is 75m and the base of triangle is 150m, the angle between each side is 0 degrees. Thus, this is not possible for triangle of these measurements to exist. This fact can be proved by trigonometry.

Adj

Cos-1q =

Hyp

75

Cos-1q =

75

q = 0

Figure 2:

Consequently, it is proved that this triangle of this particular measurement cannot exist.

AB in figure 1 is constant; therefore I will use the letter K in calculations to represent that it is a known constant. Therefore, the equation AB + BC + CA = 300 can be written as K + BC + CA = 300. We know from Phythagoras Theorem that for a right-angled triangle, like the triangle ABC in figure 1 K2 + AC2 = BC2 . To find the values of BC and CA, we can solve these two equations simultaneously:

AC + BC + AB = 300

ÞAC + BC + K = 300

AC2 = BC2 – K2

Þ AC = 300 - BC – K

Þ (AC)2 = (300 – BC –K)2

(300 – BC –K)2 = BC2 – K2

[(300 – K) - BC]2 = BC2 – K2

(300 – K)2 - 2 (300 – K) BC + BC2 = BC2 – K2

3002 – 600K + K2 – 2BC (300 – K) = - K2

2K2 – 600K + 3002 = 2BC (300 – K)

Therefore, BC = 2K2 – 600K + 3002 / 600 – 2K

Thus AC can be found, using the formula AC= 300 – BC – K.

From the above derived formulas we can find the distances for each stretch of the course. This information can be used to find the time taken to complete that particular stretch of the course. The time taken for each of the three stretches will be added to give the total time it will take to complete the course. We have to find the velocity at which the canoes travels on each stretch of the course, the missing part the velocity can be found, we know distance, thus we can substitute into the equation Time = Distance / Velocity and find velocity. This can be achieved by using scale velocity diagrams. The following are the procedures that need to be taken in order to do the scale drawings.

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STRETCH AB

The model has to be convenient for the canoeists. The current of the sea is an important factor and we have to take it into account, i.e. the effect of the prevailing current. The prevailing current is a constant opposing force. The canoe will be pushed away from its path, regardless of the direction it is moving in.

Thus, it is meaningful to travel the path AB in figure 1 from left to right where the velocity of the canoe (4ms-1) and the prevailing current (2ms-1) would be added together. Thus the resultant velocity on the stretch ...

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