phys-1600/2000phys-1600/2000 iv2 angular and linear variablesnebraska wesleyan universityfall...
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![Page 1: PHYS-1600/2000PHYS-1600/2000 IV2 Angular and Linear VariablesNEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015 DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 11 1 [Insert](https://reader035.vdocument.in/reader035/viewer/2022062408/56649efd5503460f94c106b8/html5/thumbnails/1.jpg)
PHYS-1600/2000 IV2 Angular and Linear Variables NEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015
DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 111
[Insert Puzzler Here]
![Page 2: PHYS-1600/2000PHYS-1600/2000 IV2 Angular and Linear VariablesNEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015 DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 11 1 [Insert](https://reader035.vdocument.in/reader035/viewer/2022062408/56649efd5503460f94c106b8/html5/thumbnails/2.jpg)
PHYS-1600/2000 IV2 Angular and Linear Variables NEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015
DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 1122
ANNOUNCEMENTS
ITEM DURATION START
Introductory Concept Survey (Individual) 0:10 0:00
Initial Kinematic Analysis of Rotating Plate 0:20 0:10
Relationship Between Linear and Angular Variables 0:20 0:30
Deriving Formulas for Linear Acceleration (middle of p. 3) 0:15 0:50
Complete Kinematic Analysis of Points A and B 0:25 1:05
Survey Re-vote (Group Discussion Mode) 0:10 1:30
Dismissal 1:40
AGENDA
![Page 3: PHYS-1600/2000PHYS-1600/2000 IV2 Angular and Linear VariablesNEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015 DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 11 1 [Insert](https://reader035.vdocument.in/reader035/viewer/2022062408/56649efd5503460f94c106b8/html5/thumbnails/3.jpg)
PHYS-1600/2000 IV2 Angular and Linear Variables NEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015
DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 113
1 of 3Boxes A and B are sitting on the platform of a merry-go-round, held by static friction. B is twice as far from the axis of rotation as A. The merry-go-round is accelerating in an angular sense. The magnitude of the centripetal acceleration experienced by B is
1. Zero.2. Half that of A.3. Equal to that of A.4. Twice that of A.5. Four times that of A.
B
A
![Page 4: PHYS-1600/2000PHYS-1600/2000 IV2 Angular and Linear VariablesNEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015 DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 11 1 [Insert](https://reader035.vdocument.in/reader035/viewer/2022062408/56649efd5503460f94c106b8/html5/thumbnails/4.jpg)
PHYS-1600/2000 IV2 Angular and Linear Variables NEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015
DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 114
2 of 3Boxes A and B are sitting on the platform of a merry-go-round, held by static friction. B is twice as far from the axis of rotation as A. The merry-go-round is accelerating in an angular sense. The magnitude of the tangential acceleration experienced by B is
1. Zero.2. Half that of A.3. Equal to that of A.4. Twice that of A.5. Four times that of A.
B
A
![Page 5: PHYS-1600/2000PHYS-1600/2000 IV2 Angular and Linear VariablesNEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015 DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 11 1 [Insert](https://reader035.vdocument.in/reader035/viewer/2022062408/56649efd5503460f94c106b8/html5/thumbnails/5.jpg)
PHYS-1600/2000 IV2 Angular and Linear Variables NEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015
DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 115
3 of 3
The box is sitting on the platform of a merry-go-round, held by static friction. The merry-go-round is accelerating in an angular sense. The linear acceleration vector is best represented by
1. 2.
3. 4.
a
a
a
a
![Page 6: PHYS-1600/2000PHYS-1600/2000 IV2 Angular and Linear VariablesNEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015 DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 11 1 [Insert](https://reader035.vdocument.in/reader035/viewer/2022062408/56649efd5503460f94c106b8/html5/thumbnails/6.jpg)
PHYS-1600/2000 IV2 Angular and Linear Variables NEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015
DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 1166
ANNOUNCEMENTS
ITEM DURATION START
Introductory Concept Survey (Individual) 0:10 0:00
Initial Kinematic Analysis of Rotating Plate 0:20 0:10
Relationship Between Linear and Angular Variables 0:20 0:30
Deriving Formulas for Linear Acceleration (middle of p. 3) 0:15 0:50
Complete Kinematic Analysis of Points A and B 0:25 1:05
Survey Re-vote (Group Discussion Mode) 0:10 1:30
Dismissal 1:40
AGENDA
![Page 7: PHYS-1600/2000PHYS-1600/2000 IV2 Angular and Linear VariablesNEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015 DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 11 1 [Insert](https://reader035.vdocument.in/reader035/viewer/2022062408/56649efd5503460f94c106b8/html5/thumbnails/7.jpg)
PHYS-1600/2000 IV2 Angular and Linear Variables NEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015
DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 117
IV2 Exit Homework Problem #1
![Page 8: PHYS-1600/2000PHYS-1600/2000 IV2 Angular and Linear VariablesNEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015 DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 11 1 [Insert](https://reader035.vdocument.in/reader035/viewer/2022062408/56649efd5503460f94c106b8/html5/thumbnails/8.jpg)
PHYS-1600/2000 IV2 Angular and Linear Variables NEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015
DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 118
IV2 Exit Homework Problem #2
![Page 9: PHYS-1600/2000PHYS-1600/2000 IV2 Angular and Linear VariablesNEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015 DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 11 1 [Insert](https://reader035.vdocument.in/reader035/viewer/2022062408/56649efd5503460f94c106b8/html5/thumbnails/9.jpg)
PHYS-1600/2000 IV2 Angular and Linear Variables NEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015
DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 119
1 of 3Boxes A and B are sitting on the platform of a merry-go-round, held by static friction. B is twice as far from the axis of rotation as A. The merry-go-round is accelerating in an angular sense. The magnitude of the centripetal acceleration experienced by B is
1. Zero.2. Half that of A.3. Equal to that of A.4. Twice that of A.5. Four times that of A.
B
A
![Page 10: PHYS-1600/2000PHYS-1600/2000 IV2 Angular and Linear VariablesNEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015 DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 11 1 [Insert](https://reader035.vdocument.in/reader035/viewer/2022062408/56649efd5503460f94c106b8/html5/thumbnails/10.jpg)
PHYS-1600/2000 IV2 Angular and Linear Variables NEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015
DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 1110
2 of 3Boxes A and B are sitting on the platform of a merry-go-round, held by static friction. B is twice as far from the axis of rotation as A. The merry-go-round is accelerating in an angular sense. The magnitude of the tangential acceleration experienced by B is
1. Zero.2. Half that of A.3. Equal to that of A.4. Twice that of A.5. Four times that of A.
B
A
![Page 11: PHYS-1600/2000PHYS-1600/2000 IV2 Angular and Linear VariablesNEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015 DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 11 1 [Insert](https://reader035.vdocument.in/reader035/viewer/2022062408/56649efd5503460f94c106b8/html5/thumbnails/11.jpg)
PHYS-1600/2000 IV2 Angular and Linear Variables NEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015
DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 1111
3 of 3
The box is sitting on the platform of a merry-go-round, held by static friction. The merry-go-round is accelerating in an angular sense. The linear acceleration vector is best represented by
1. 2.
3. 4.
a
a
a
a
![Page 12: PHYS-1600/2000PHYS-1600/2000 IV2 Angular and Linear VariablesNEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015 DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 11 1 [Insert](https://reader035.vdocument.in/reader035/viewer/2022062408/56649efd5503460f94c106b8/html5/thumbnails/12.jpg)
PHYS-1600/2000 IV2 Angular and Linear Variables NEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015
DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 1112
1 4 1 4 1 4 1 4
2 5 2 5 2 5 2 5
3 3 3 3
PROJECTION SCREEN
6 6 6 6
IV2: HAND IN TODAY’S ACTIVITIES SHEETS