Page 2 - Combined_57_OCR
P. 2

Page 2.

                 Performance of 1969 Dodge Charger 500 at Daytona International
                 Speedway

                 Discussion (cont3 d)

                 The cir, end as result is somewhat affected by the 10-15 mph., wind
                 conditions that existed during the test.

                        For analysis the particular lap chosen was the third lap of
                 test number 10, which had a lap speed of 136.119 mph. Curve sheet
                 #1 gives the epgine speed and yaw measured fo'r this lap together
                 with car speed and car acceleration derived from the engine speed.
                 The engine speed data has been smoothed to eliminate some roughnes
                 but the small amount of wheel spin that occiirs coming out of turn 2
                 and turn 4 has been left in. The wheelspin in these two locations
                 occurs during almost all of the laps recorded. It occurs just at
                 the end of the banking.

                        During the particular lap plotted the wind was about 10-15 mph.
                 blowing from an easterly direction. This accounts for the greater
                 speed on the front straight than the back straight. The wind also
                 accounts for difference in handling of the car between the two turns.
                 The yaw trace is reproduced only slightly smoothed! with the lower
                 frequency oscilatiohs left in. 'These yaw variations vary from lap
                 to lap, but similar frequency yaw changes"are present in each lap.
                 In all cases the yaw angles measured are less in turns 1 and 2 than
                 in 3 and 4. This is in agreement with the driver" s comments that the
                 car had more understeer in turns 1 and 2 during the whole test period.
                 In turns 3 and 4 the yaw angle is higher since an oversteer condition
                 was experienced there. Also in turns 3 and 4 the amplitude of the
                 oscilations in yaw are greater, possibly indicating that the car was
                 closer to breaking loose completely. With the wind direction as it
                 was during most of the test the number 3 and 4 turns are well shielded
                 from the wind by the banking, sc that the measured yaw is probably
                 very close to the actual yaw. In turns 1 and 2 the car experiences
                 considerable wind effects, so the yaw angles measured here are less
                 reliable. The yaw angles shown for the tri-oval turn are consider­
                 ably less than for the other turns..
                        Figure 2 shows the forces acting on the car for the lap plotted-,
                 as well as the locations on the race track. The top plot on the
                 curve shows the banking angle around the race track as well as the
                 locations of the straights, turns and transitions. This is from data
                 on the design of the race track obtained from Mr. C.H. Moneypenny the
                 truck designer. Also on the same sheet are plots of the normal and
                 lateral forces acting on the car during the lap. These are the total
                  gravitational forces acting on the car perpendicular and parallel
                 to the road surface at a given point. These are calculated from the
                 track data and the speed data and from data on the assumed line that
                 the car travels entering and leaving the turns. It will be noted that
                 the normal force exceeds 9000 lbs. entering turn number 1. The forces
                 entering turn 3 are slightly less due to the lower speed at this point
                 because of the headwind on the back straight. Also plotted on this
                 sheet is the ratio of the lateral force to the normal force. Tire
                 slip angle and car yaw angle are generally a function of this ratio.
                 The ratio is the equivalent of the lateral acceleration in terms of
                 ’’G" as measured on a flat turn.
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