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initial conditions t1 = 0 x1 v1 = u final conditions t2 = t x2 v2 = v

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Presentation on theme: "initial conditions t1 = 0 x1 v1 = u final conditions t2 = t x2 v2 = v"โ€” Presentation transcript:

1 initial conditions t1 = 0 x1 v1 = u final conditions t2 = t x2 v2 = v
origin always show an arrow for +X direction always specify the origin v < 0 a < 0 v > 0 a < 0 v < 0 a > 0 v > 0 a > 0 +X x < 0 x > 0 x = 0 origin

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4 Z ๐‘˜ O(0,0,0) ๐‘— Y ๐‘– X

5 P(1, 2) ๐‘  ๐‘ƒ [m] O ๐œƒ ๐‘ƒ ๐œƒ ๐‘„ ๐œƒ ๐‘… ๐‘  ๐‘… R(-4, -3) Q(3, -4) ๐‘  ๐‘„ [m]

6 P(1, 2) [m] O ๐‘  ๐‘… ๐‘  ๐‘„ ๐‘  ๐‘…๐‘„ R(-4, -3) Q(3, -4) [m]

7 P(1, 2) ๐‘  ๐‘ƒ [m] ๐‘  ๐‘ƒ๐‘„ O R(-4, -3) ๐‘  ๐‘„ Q(3, -4) [m]

8 Y ๐‘  ๐‘— ๐œƒ ๐‘– O(0, 0) X

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10 P(1, 2) ๐‘  ๐‘…๐‘ƒ ๐‘  ๐‘ƒ ๐‘  ๐‘„๐‘ƒ ๐‘  ๐‘… ๐‘  ๐‘„ ๐‘  ๐‘…๐‘„ Q(3, -4) R(-4, -3)

11 P(1, 2) Q(3, -4) R(-4, -3)

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13 head tail ๐‘ฃ v v

14 ๐ต - ๐ด 2 ๐ด

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17 ๐‘› ๐‘›

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19 Y X Initial position of crate final position of crate ๐น ๐‘ ๐น ๐‘ ๐น ๐‘‡ ๐น ๐‘‡
๐น ๐‘ ๐น ๐‘ ๐น ๐‘‡ ๐น ๐‘‡ X ๐น ๐บ ๐น ๐บ ๐‘  displacement of crate ๐น ๐‘‡ ๐œ™

20 applied force ๐น Origin: pivot point ๐‘Ÿ lever arm vector ๐‘› ๐น ๐‘Ÿ ๐œƒ

21 v = 0 x v v < 0 v > 0 t t a = 0 v a a < 0 a > 0 t t
velocity = slope of tangent x/t graph change in displacement = area under v/t graph v a = 0 a a < 0 a > 0 t t acceleration = slope of tangent v/t graph change in velocity = area under a/t graph

22 ๏‚บ + a > 0 a > 0 F1 m F2 m m g = +9.8 m.s-2 r FC
centripetal acceleration aC directed towards centre of circle v centripetal force FC directed towards centre of circle Magnitude of v is constant Change in direction of v is always directed to centre of circle

23 + v > 0 v < 0 m m p = m v > 0 p = m v < 0 v1 = u force F acts time ๏„t v2 = v m m initial momentum p1 final momentum p2

24 + v > 0 v < 0 m m p = m v > 0 p = m v < 0 v1 = u force F acts over displacement ๏„s v2 = v m m initial KE EK1 final KE EK2 work done on object W = F ๏„s

25 - +Q V d qe V = 0 -Q electric field is uniform between charged plates
electron accelerated by electric field

26 vorb2 r2 vorb1 r1 T2 T1 M

27 A I ammeter ๏ฅ R V voltmeter

28 slope = 0 ๏†Bmax T/4 max neg slope max pos slope

29 coil rotates clockwise
current I (out) side views of coil A B A A A A A A current I (in) 0o ๏ฑ ๏ƒ  180o 360o 90o 270o torque always acts to produce a clockwise rotation T = 5.0 ms

30 uniform magnetic field B into page
v negative charge q enters uniform B-field FB causes a change in direction, no change in speed since FB acts at right angle to v r force F on charge always directed to centre of circle Circular motion: Magnetic force = Centripetal force


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