matt brady james gallo jon lesner alex quehl engineering-design 100, section 10 group 2 xinli wu the...
TRANSCRIPT
2-LASER TRIPLE-CHECK SYSTEM
Matt BradyJames GalloJon LesnerAlex Quehl
Engineering-Design 100, Section 10Group 2Xinli Wu
The Pennsylvania State University
The Problem
Need for a more accurate velocity measurement allows for: Higher-quality picture (micron tolerances) Better handling of paper while being printed
Due to wear and tear, centripetal velocity of rollers changes as time progresses
Without accurate velocity, distorted picture is likely
The Solution
Design measuring paper velocity Measures velocity 3 times:
Time beam of laser 1 is blocked from sensor 1 Time beam of laser 2 is blocked from sensor 2 Time between lasers
Paper length and distance between lasers are both constant
Time /distance = velocity Finds the mean of all 3, minimizing chance for
a flawed calculation
The Prototype
2 rollers in front 2 rollers in back 2 lasers located between front and back
rollers Fixed distance is needed to find velocity Sensor corresponding to each laser Baffle to guide the paper Framing
Example
Internal clock able to measure to the millisecond
First, it takes 4 time measurements, then calculates 3 velocities, using d /∆t (distance / change in time), where: d1 = d2 = 279.4 mm (i.e., length of paper) d3 = 63.5 mm (i.e., distance between sensors) ∆t1 = tb – ta
∆t2 = td – tc
∆t3 = tc - ta
Example (Cont.)
Start Time of Sensor 1 (ta)
End Time of Sensor 1 (tb)
Start Time of Sensor 2 (tc)
End Time of Sensor 2 (td)
3:06:23:125 3:06:23:741 3:06:23:267 3:06:23:893
Velocity 1 Velocity 2 Velocity 3 Mean Velocity
279.4 mm 0.616 s
279.4 mm0.626 s
63.5 mm0.142 s
v1 + v2 + v3
3
453.57 mm/s 446.33 mm/s 447.18 mm/s
449.03 mm/s
∆t1 = tb - ta
∆t2 = td – tc
∆t3 = tc - ta
0.616 s 0.626 s 0.142 s
Conclusion
Optimal accuracy, considering the relatively small number of resources used
Eliminates the risk that comes with taking just one measurement
Ideal for a printer with such a great need for super-precise calculations