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Describes gallilean transformations of reference frames.

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FRAMES OF REFERENCE –IIROTATING FRAMES

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FRAMES OF REFERENCE –IIROTATING FRAMES

1 Galilean Transformations

2 Galilean Relativity

3 Non-inertial Frames

Uniformly accelerated frames

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Motion in Rotating Frames

First, an important result:

Frames of Reference Rotating frames

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Motion in Rotating Frames

First, an important result:

* 2* 2* 0* .05* 0.1* 0.15001* 0.20001* 0.25002* 0.30002* 0.35002* 0.400

Frames of Reference Rotating frames

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Motion in Rotating Frames

First, an important result:

* 2* 2* 0* .05* 0.1* 0.15001* 0.20001* 0.25002* 0.30002* 0.35002* 0.400Frames of Reference Rotating frames

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Motion in Rotating Frames

First, an important result:

* 2* 2* 0* .05* 0.1* 0.15001* 0.20001* 0.25002* 0.30002* 0.35002* 0.400Frames of Reference Rotating frames

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Motion in Rotating Frames

First, an important result:

* 2* 2* 0* .05* 0.1* 0.15001* 0.20001* 0.25002* 0.30002* 0.35002* 0.400Frames of Reference Rotating frames

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Motion in Rotating Frames

First, an important result:

* 2* 2* 0* .05* 0.1* 0.15001* 0.20001* 0.25002* 0.30002* 0.35002* 0.400Frames of Reference Rotating frames

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Motion in Rotating Frames

First, an important result:

* 2* 2* 0* .05* 0.1* 0.15001* 0.20001* 0.25002* 0.30002* 0.35002* 0.400Frames of Reference Rotating frames

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Motion in Rotating Frames

First, an important result:

* 2* 2* 0* .05* 0.1* 0.15001* 0.20001* 0.25002* 0.30002* 0.35002* 0.400Frames of Reference Rotating frames

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Motion in Rotating Frames

First, an important result:

* 2* 2* 0* .05* 0.1* 0.15001* 0.20001* 0.25002* 0.30002* 0.35002* 0.400Frames of Reference Rotating frames

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Motion in Rotating Frames

First, an important result:

* 2* 2* 0* .05* 0.1* 0.15001* 0.20001* 0.25002* 0.30002* 0.35002* 0.400Frames of Reference Rotating frames

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Motion in Rotating Frames

Rotating frame (x, y, z), coincident with inertial frame (x,y,z) at t

rotate0.pdf

Frames of Reference Rotating frames

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Motion in Rotating Frames

Rotating frame (x, y, z), coincident with inertial frame (x,y,z) at t

Vector

−→

B (t) on x-z plane (Say)

rotate0.pdf

Frames of Reference Rotating frames

M i i R i F

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Motion in Rotating Frames

Rotating frame (x, y, z), coincident with inertial frame (x,y,z) at t

Vector

−→

B (t) on x-z plane (Say)At t + ∆t,

rotateS0.pdf

Frames of Reference Rotating frames

M ti i R t ti F

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Motion in Rotating Frames

Rotating frame (x, y, z), coincident with inertial frame (x,y,z) at t

Vector

−→

B (t) on x-z plane (Say)At t + ∆t,

In inertial frame,

∆−→B =

−→B (t + ∆t) −

−→B (t)

rotateS1.pdf

Frames of Reference Rotating frames

M ti i R t ti F

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Motion in Rotating Frames

Rotating frame (x, y, z), coincident with inertial frame (x,y,z) at t

Vector

−→

B (t) on x-z plane (Say)At t + ∆t,

In inertial frame,

∆−→B =

−→B (t + ∆t) −

−→B (t)

In rotating frame, rotateS’0.pdf

Frames of Reference Rotating frames

M ti i R t ti F

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Motion in Rotating Frames

Rotating frame (x, y, z), coincident with inertial frame (x,y,z) at t

Vector

−→

B (t) on x-z plane (Say)At t + ∆t,

In inertial frame,

∆−→B =

−→B (t + ∆t) −

−→B (t)

In rotating frame, rotateS’1.pdf

Frames of Reference Rotating frames

Motion in Rotating Frames

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Motion in Rotating Frames

Rotating frame (x, y, z), coincident with inertial frame (x,y,z) at t

Vector

−→

B (t) on x-z plane (Say)At t + ∆t,

In inertial frame,

∆−→B =

−→B (t + ∆t) −

−→B (t)

In rotating frame,

−→

B

=

−→

B (t + ∆t) −

−→

B

(t)

rotateS’1.pdf

Frames of Reference Rotating frames

Motion in Rotating Frames

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Motion in Rotating Frames

Rotating frame (x, y, z), coincident with inertial frame (x,y,z) at t

Vector

−→

B (t) on x-z plane (Say)At t + ∆t,

In inertial frame,

∆−→B =

−→B (t + ∆t) −

−→B (t)

In rotating frame,

−→

B

=

−→

B (t + ∆t) −

−→

B

(t)

∴ ∆−→B = ∆

−→B

+ [−→B

(t) −−→B (t)]

rotateS’1.pdf

Frames of Reference Rotating frames

Motion in Rotating Frames

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Motion in Rotating Frames

Rotating frame (x, y, z), coincident with inertial frame (x,y,z) at t

Vector

−→

B (t) on x-z plane (Say)At t + ∆t,

In inertial frame,

∆−→B =

−→B (t + ∆t) −

−→B (t)

In rotating frame,

−→

B

=

−→

B (t + ∆t) −

−→

B

(t)

∴ ∆−→B = ∆

−→B

+ [−→B

(t) −−→B (t)]

−→B rotated with frame

rotate5.pdf

Frames of Reference Rotating frames

Motion in Rotating Frames

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Motion in Rotating Frames

Rotating frame (x, y, z), coincident with inertial frame (x,y,z) at t

Vector

−→B

(t) on

x-z

plane (Say)At t + ∆t,

In inertial frame,

∆−→B =

−→B (t + ∆t) −

−→B (t)

In rotating frame,

−→

B

=

−→

B (t + ∆t) −

−→

B

(t)

∴ ∆−→B = ∆

−→B

+ [−→B

(t) −−→B (t)]

= (−→Ω ×

−→B )∆t

rotate6.pdf

Frames of Reference Rotating frames

Motion in Rotating Frames

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Motion in Rotating Frames

Rotating frame (x, y, z), coincident with inertial frame (x,y,z) at t

Vector−→B

(t)

on x-z plane (Say)

At t + ∆t,

In inertial frame,

∆−→B =

−→B (t + ∆t) −

−→B (t)

In rotating frame,

−→

B

=

−→

B (t + ∆t) −

−→

B

(t)

∴ ∆−→B = ∆

−→B

+ [−→B

(t) −−→B (t)]

= (−→Ω ×

−→B )∆t

∆−→B

∆t

= ∆−→B

∆t

+ Ω ×−→B

rotate7.pdf

Frames of Reference Rotating frames

Velocity and Acceleration in Rotating Frames

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Velocity and Acceleration in Rotating Frames

Frames of Reference Rotating frames

Velocity and Acceleration in Rotating Frames

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Velocity and Acceleration in Rotating Frames

d−→B

dt

in

= d−→B

dt

rot

+−→Ω ×

−→B

Frames of Reference Rotating frames

Velocity and Acceleration in Rotating Frames

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Velocity and Acceleration in Rotating Frames

d−→B

dt

in

= d−→B

dt

rot

+−→Ω ×

−→B

Put−→B = r, vin = vrot +

−→Ω × r

Frames of Reference Rotating frames

Velocity and Acceleration in Rotating Frames

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Velocity and Acceleration in Rotating Frames

d−→B

dt

in

= d−→B

dt

rot

+−→Ω ×

−→B

Put−→B = r, vin = vrot +

−→Ω × r

ain = dv

dt

in

=

Frames of Reference Rotating frames

Velocity and Acceleration in Rotating Frames

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Velocity and Acceleration in Rotating Frames

d−→B

dt

in

= d−→B

dt

rot

+−→Ω ×

−→B

Put−→B = r, vin = vrot +

−→Ω × r

ain = dv

dt

in

= d

dt(vrot +

−→Ω × r)

rot

+−→Ω × (vrot +

−→Ω

Frames of Reference Rotating frames

Velocity and Acceleration in Rotating Frames

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Velocity and Acceleration in Rotating Frames

d−→B

dt

in

= d−→B

dt

rot

+−→Ω ×

−→B

Put−→B = r, vin = vrot +

−→Ω × r

ain = dv

dt

in

= d

dt(vrot +

−→Ω × r)

rot

+−→Ω × (vrot +

−→Ω

Assume Ω constant,

Frames of Reference Rotating frames

Velocity and Acceleration in Rotating Frames

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Velocity and Acceleration in Rotating Frames

d−→B

dt

in

= d−→B

dt

rot

+−→Ω ×

−→B

Put−→B = r, vin = vrot +

−→Ω × r

ain = dv

dt

in

= d

dt(vrot +

−→Ω × r)

rot

+−→Ω × (vrot +

−→Ω

Assume Ω constant,

ain =

Frames of Reference Rotating frames

Velocity and Acceleration in Rotating Frames

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e oc ty a d cce e at o otat g a es

d−→B

dt

in

= d−→B

dt

rot

+−→Ω ×

−→B

Put−→B = r, vin = vrot +

−→Ω × r

ain = dv

dt

in

= d

dt(vrot +

−→Ω × r)

rot

+−→Ω × (vrot +

−→Ω

Assume Ω constant,

ain = dv

dt

rot

Frames of Reference Rotating frames

Velocity and Acceleration in Rotating Frames

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y g

d−→B

dt

in

= d−→B

dt

rot

+−→Ω ×

−→B

Put−→B = r, vin = vrot +

−→Ω × r

ain = dv

dt

in

= d

dt(vrot +

−→Ω × r)

rot

+−→Ω × (vrot +

−→Ω

Assume Ω constant,

ain = dv

dt

rot

+−→Ω ×

dr

dt

rot

Frames of Reference Rotating frames

Velocity and Acceleration in Rotating Frames

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y g

d−→B

dt

in

= d−→B

dt

rot

+−→Ω ×

−→B

Put−→B = r, vin = vrot +

−→Ω × r

ain = dv

dt

in

= d

dt(vrot +

−→Ω × r)

rot

+−→Ω × (vrot +

−→Ω

Assume Ω constant,

ain = dv

dt

rot

+−→Ω ×

dr

dt

rot

+−→Ω × vrot

Frames of Reference Rotating frames

Velocity and Acceleration in Rotating Frames

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y g

d−→B

dt

in

= d−→B

dt

rot

+−→Ω ×

−→B

Put−→B = r, vin = vrot +

−→Ω × r

ain = dv

dt

in

= d

dt(vrot +

−→Ω × r)

rot

+−→Ω × (vrot +

−→Ω

Assume Ω constant,

ain = dv

dt

rot

+−→Ω ×

dr

dt

rot

+−→Ω × vrot +

−→Ω × (

−→Ω ×

Frames of Reference Rotating frames

Velocity and Acceleration in Rotating Frames

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y g

d−→B

dt

in

= d−→B

dt

rot

+−→Ω ×

−→B

Put−→B = r, vin = vrot +

−→Ω × r

ain = dv

dt

in

= d

dt(vrot +

−→Ω × r)

rot

+−→Ω × (vrot +

−→Ω

Assume Ω constant,

ain = dv

dt

rot

+−→Ω ×

dr

dt

rot

+−→Ω × vrot +

−→Ω × (

−→Ω ×

= arot +

Frames of Reference Rotating frames

Velocity and Acceleration in Rotating Frames

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d−→B

dt

in

= d−→B

dt

rot

+−→Ω ×

−→B

Put−→B = r, vin = vrot +

−→Ω × r

ain = dv

dt

in

= d

dt(vrot +

−→Ω × r)

rot

+−→Ω × (vrot +

−→Ω

Assume Ω constant,

ain = dv

dt

rot

+−→Ω ×

dr

dt

rot

+−→Ω × vrot +

−→Ω × (

−→Ω ×

= arot + 2−→Ω × vrot

Frames of Reference Rotating frames

Velocity and Acceleration in Rotating Frames

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d−→B

dt

in

= d−→B

dt

rot

+−→Ω ×

−→B

Put−→B = r, vin = vrot +

−→Ω × r

ain = dv

dt

in

= d

dt(vrot +

−→Ω × r)

rot

+−→Ω × (vrot +

−→Ω

Assume Ω constant,

ain = dv

dt

rot

+−→Ω ×

dr

dt

rot

+−→Ω × vrot +

−→Ω × (

−→Ω ×

= arot + 2−→Ω × vrot +

−→Ω × (

−→Ω × r)

Frames of Reference Rotating frames

Velocity and Acceleration in Rotating Frames

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d−→B

dt

in

= d−→B

dt

rot

+−→Ω ×

−→B

Put−→B = r, vin = vrot +

−→Ω × r

ain = dv

dt

in

= d

dt(vrot +

−→Ω × r)

rot

+−→Ω × (vrot +

−→Ω

Assume Ω constant,

ain = dv

dt

rot

+−→Ω ×

dr

dt

rot

+−→Ω × vrot +

−→Ω × (

−→Ω ×

= arot + 2−→Ω × vrot +

−→Ω × (

−→Ω × r)

CoriolisFrames of Reference Rotating frames

Velocity and Acceleration in Rotating Frames

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d−→B

dt

in

= d−→B

dt

rot

+−→Ω ×

−→B

Put−→B = r, vin = vrot +

−→Ω × r

ain = dv

dt

in

= d

dt(vrot +

−→Ω × r)

rot

+−→Ω × (vrot +

−→Ω

Assume Ω constant,

ain = dv

dt

rot

+−→Ω ×

dr

dt

rot

+−→Ω × vrot +

−→Ω × (

−→Ω ×

= arot + 2−→Ω × vrot +

−→Ω × (

−→Ω × r)

Coriolis CentrifugalFrames of Reference Rotating frames

Apparent Forces in a rotating system

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Physical force on system:−→F =

−→F in = main

Frames of Reference Rotating frames

Apparent Forces in a rotating system

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Physical force on system:−→F =

−→F in = main

Force observed in rotating frame:

−→F rot = main −2m

−→Ω × vrot −m

−→Ω × (

−→Ω × r)

Frames of Reference Rotating frames

Apparent Forces in a rotating system

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Physical force on system:−→F =

−→F in = main

Force observed in rotating frame:

−→F rot = main −2m

−→Ω × vrot −m

−→Ω × (

−→Ω × r)

=−→F +

−→F fict

Frames of Reference Rotating frames

Apparent Forces in a rotating system

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Physical force on system:−→F =

−→F in = main

Force observed in rotating frame:

−→F rot = main −2m

−→Ω × vrot −m

−→Ω × (

−→Ω × r)

=−→F +

−→F fict

(a) Coriolis force

when the mass is moving in the rotating

frame

Frames of Reference Rotating frames

Apparent Forces in a rotating system

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Physical force on system:−→F =

−→F in = main

Force observed in rotating frame:

−→F rot = main −2m

−→Ω × vrot −m

−→Ω × (

−→Ω × r)

=−→F +

−→F fict

(a) Coriolis force

when the mass is moving in the rotating

frame

(b) Centrifugal Force

evident even when the mas

Frames of Reference Rotating frames

Centrifugal force

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Is familiar to us!

centrifugal0.pdf

Frames of Reference Rotating frames Centrifu

Centrifugal force

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Is familiar to us!

−→Ω × (

−→Ω × r) =

centrifugal1.pdf

Frames of Reference Rotating frames Centrifu

Centrifugal force

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Is familiar to us!

−→Ω × (

−→Ω × r) =

centrifugal2.pdf

Frames of Reference Rotating frames Centrifu

Centrifugal force

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Is familiar to us!

−→Ω × (

−→Ω × r) = −Ω2ρρ

centrifugal3.pdf

Frames of Reference Rotating frames Centrifu

Centrifugal force

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Is familiar to us!

−→Ω × (

−→Ω × r) = −Ω2ρρ

−→F centrifugal = mΩ2ρρ

centrifugal4.pdf

Frames of Reference Rotating frames Centrifu

Centrifugal force

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Is familiar to us!

−→Ω × (

−→Ω × r) = −Ω2ρρ

−→F centrifugal = mΩ2ρρ

directed away from the

axiscentrifugal4.pdf

Frames of Reference Rotating frames Centrifu

Coriolis force

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−→F cor = −2m

−→Ω × v

Gustave_corioli

Frames of Reference Rotating frames Corioli

Coriolis force

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−→F cor = −2m

−→Ω × v

corF0.pdf

Gustave_corioli

Frames of Reference Rotating frames Corioli

Coriolis force

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−→F cor = −2m

−→Ω × v

corF1.pdf

Gustave_corioli

Frames of Reference Rotating frames Corioli

Coriolis force

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−→F cor = −2m

−→Ω × v

corF2.pdf

Gustave_corioli

Frames of Reference Rotating frames Corioli

Coriolis force

Page 55: Ref Frames 1

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−→F cor = −2m

−→Ω × v

corF3.pdf

Gustave_corioli

Frames of Reference Rotating frames Corioli

Coriolis force

Page 56: Ref Frames 1

7/17/2019 Ref Frames 1

http://slidepdf.com/reader/full/ref-frames-1 56/58

−→F cor = −2m

−→Ω × v

corF.pdf

Magnitude:

F cor = 2mΩv⊥,

Gustave_corioli

Frames of Reference Rotating frames Corioli

Coriolis force

Page 57: Ref Frames 1

7/17/2019 Ref Frames 1

http://slidepdf.com/reader/full/ref-frames-1 57/58

−→F cor = −2m

−→Ω × v

corF.pdf

Magnitude:

F cor = 2mΩv⊥,

Direction: er endicular

Gustave_corioli

Frames of Reference Rotating frames Corioli

Coriolis force

Page 58: Ref Frames 1

7/17/2019 Ref Frames 1

http://slidepdf.com/reader/full/ref-frames-1 58/58

−→F cor = −2m

−→Ω × v

corF.pdf

Magnitude:

F cor = 2mΩv⊥,

Direction: er endicular

Gustave_corioli

On a merry-go-round in the

Coriolis was shaken with friDespite how he walked

’Twas like he was stalked

By some fiend always pu

him right!

– David Morin, Eric Zaslow, E liza be th Ha

Frames of Reference Rotating frames Corioli