x2 t07 04 uniform circular motion (2010)

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Acceleration with Uniform Circular Motion

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Page 1: X2 T07 04 uniform circular motion (2010)

Acceleration with Uniform Circular Motion

Page 2: X2 T07 04 uniform circular motion (2010)

Acceleration with Uniform Circular Motion

Uniform circular motion is when a particle moves with constant angular velocity.

Page 3: X2 T07 04 uniform circular motion (2010)

Acceleration with Uniform Circular Motion

Uniform circular motion is when a particle moves with constant angular velocity. constantbealsoocity willlinear veltheofmagnitude the

Page 4: X2 T07 04 uniform circular motion (2010)

Acceleration with Uniform Circular Motion

Uniform circular motion is when a particle moves with constant angular velocity.

Or

A

constantbealsoocity willlinear veltheofmagnitude the

Page 5: X2 T07 04 uniform circular motion (2010)

Acceleration with Uniform Circular Motion

Uniform circular motion is when a particle moves with constant angular velocity.

Or

A

P

constantbealsoocity willlinear veltheofmagnitude the

A particle moves from A

to P with constant angular velocity.

Page 6: X2 T07 04 uniform circular motion (2010)

Acceleration with Uniform Circular Motion

Uniform circular motion is when a particle moves with constant angular velocity.

Or

A

P

constantbealsoocity willlinear veltheofmagnitude the

A particle moves from A

to P with constant angular velocity.

The acceleration of the particle is the change in velocity with respect to time.

Page 7: X2 T07 04 uniform circular motion (2010)

Acceleration with Uniform Circular Motion

Uniform circular motion is when a particle moves with constant angular velocity.

Or

A

P

v

constantbealsoocity willlinear veltheofmagnitude the

A particle moves from A

to P with constant angular velocity.

The acceleration of the particle is the change in velocity with respect to time.

Page 8: X2 T07 04 uniform circular motion (2010)

Acceleration with Uniform Circular Motion

Uniform circular motion is when a particle moves with constant angular velocity.

Or

A

P

v

constantbealsoocity willlinear veltheofmagnitude the

v’

A particle moves from A

to P with constant angular velocity.

The acceleration of the particle is the change in velocity with respect to time.

Page 9: X2 T07 04 uniform circular motion (2010)

Acceleration with Uniform Circular Motion

Uniform circular motion is when a particle moves with constant angular velocity.

Or

A

P

v

constantbealsoocity willlinear veltheofmagnitude the

v’

A particle moves from A

to P with constant angular velocity.

The acceleration of the particle is the change in velocity with respect to time.

v

Page 10: X2 T07 04 uniform circular motion (2010)

Acceleration with Uniform Circular Motion

Uniform circular motion is when a particle moves with constant angular velocity.

Or

A

P

v

constantbealsoocity willlinear veltheofmagnitude the

v’

A particle moves from A

to P with constant angular velocity.

The acceleration of the particle is the change in velocity with respect to time.

vv’

Page 11: X2 T07 04 uniform circular motion (2010)

Acceleration with Uniform Circular Motion

Uniform circular motion is when a particle moves with constant angular velocity.

Or

A

P

v

constantbealsoocity willlinear veltheofmagnitude the

v’

A particle moves from A

to P with constant angular velocity.

The acceleration of the particle is the change in velocity with respect to time.

vv’

v

Page 12: X2 T07 04 uniform circular motion (2010)

Acceleration with Uniform Circular Motion

Uniform circular motion is when a particle moves with constant angular velocity.

Or

A

P

v

constantbealsoocity willlinear veltheofmagnitude the

v’

A particle moves from A

to P with constant angular velocity.

The acceleration of the particle is the change in velocity with respect to time.

vv’

v

Page 13: X2 T07 04 uniform circular motion (2010)

Acceleration with Uniform Circular Motion

Uniform circular motion is when a particle moves with constant angular velocity.

Or

A

P

v

constantbealsoocity willlinear veltheofmagnitude the

v’

A particle moves from A

to P with constant angular velocity.

The acceleration of the particle is the change in velocity with respect to time.

vv’

v

OAPsimilar tois

vectorsoftriangleThis

Page 14: X2 T07 04 uniform circular motion (2010)

vv’

v

O

rA

r

Page 15: X2 T07 04 uniform circular motion (2010)

vv’

v

O

rA

Pr

rv

APv

Page 16: X2 T07 04 uniform circular motion (2010)

vv’

v

O

rA

Pr

rv

APv

rAPvv

Page 17: X2 T07 04 uniform circular motion (2010)

vv’

v

O

rA

Pr

rv

APv

rAPvv

tva

Page 18: X2 T07 04 uniform circular motion (2010)

vv’

v

O

rA

Pr

rv

APv

rAPvv

tva

trAPva

Page 19: X2 T07 04 uniform circular motion (2010)

vv’

v

O

rA

Pr

rv

APv

rAPvv

tva

trAPva

arcAPAPΔt ,0asBut,

Page 20: X2 T07 04 uniform circular motion (2010)

vv’

v

O

rA

Pr

rv

APv

rAPvv

tva

trAPva

arcAPAPΔt ,0asBut,

trarcAPva

t

0

lim

Page 21: X2 T07 04 uniform circular motion (2010)

vv’

v

O

rA

Pr

rv

APv

rAPvv

tva

trAPva

arcAPAPΔt ,0asBut,

trarcAPva

t

0

lim

tvarcAP timespeeddistance

Page 22: X2 T07 04 uniform circular motion (2010)

vv’

v

O

rA

Pr

rv

APv

rAPvv

tva

trAPva

arcAPAPΔt ,0asBut,

trarcAPva

t

0

lim

tvarcAP timespeeddistance

rv

rv

trtvva

t

t

2

2

0

0

lim

lim

Page 23: X2 T07 04 uniform circular motion (2010)

vv’

v

O

rA

Pr

rv

APv

rAPvv

tva

trAPva

arcAPAPΔt ,0asBut,

trarcAPva

t

0

lim

tvarcAP timespeeddistance

rv

rv

trtvva

t

t

2

2

0

0

lim

lim

centrethetowardsdirected

is and magnitude hasmotion

circular uniformin on acceleratithe2

rv

Page 24: X2 T07 04 uniform circular motion (2010)

rva

2

Acceleration Involved inUniform Circular Motion

Page 25: X2 T07 04 uniform circular motion (2010)

rva

2

2raOR

Acceleration Involved inUniform Circular Motion

Page 26: X2 T07 04 uniform circular motion (2010)

rva

2

2raOR

Acceleration Involved inUniform Circular Motion

Forces Involved inUniform Circular Motion

Page 27: X2 T07 04 uniform circular motion (2010)

rva

2

2raOR

Acceleration Involved inUniform Circular Motion

rmvF

2

Forces Involved inUniform Circular Motion

Page 28: X2 T07 04 uniform circular motion (2010)

rva

2

2raOR

Acceleration Involved inUniform Circular Motion

rmvF

2

2mrFOR

Forces Involved inUniform Circular Motion

Page 29: X2 T07 04 uniform circular motion (2010)

rva

2

2raOR

Acceleration Involved inUniform Circular Motion

rmvF

2

2mrFOR

Forces Involved inUniform Circular Motion

e.g. (i) (2003)A particle P

of mass m

moves with constant angular velocity

on a circle of radius r. Its position at time t

is given by;

tryrx

where,sincos

Page 30: X2 T07 04 uniform circular motion (2010)

rva

2

2raOR

Acceleration Involved inUniform Circular Motion

rmvF

2

2mrFOR

Forces Involved inUniform Circular Motion

e.g. (i) (2003)A particle P

of mass m

moves with constant angular velocity

on a circle of radius r. Its position at time t

is given by;

tryrx

where,sincos

.on acting magnitude of force radial inwardan is e that therShow a) 2

Pmr

Page 31: X2 T07 04 uniform circular motion (2010)

y

x

P

r

cosrx

sinry

Page 32: X2 T07 04 uniform circular motion (2010)

y

x

P

r

cosrx

sinry

cosrx

Page 33: X2 T07 04 uniform circular motion (2010)

y

x

P

r

cosrx

sinry

cosrx sinry

Page 34: X2 T07 04 uniform circular motion (2010)

y

x

P

r

cosrx

sinry

cosrx sinry

sin

sin

rdtdrx

Page 35: X2 T07 04 uniform circular motion (2010)

y

x

P

r

cosrx

sinry

cosrx sinry

sin

sin

rdtdrx

cos

cos

rdtdry

Page 36: X2 T07 04 uniform circular motion (2010)

y

x

P

r

cosrx

sinry

cosrx sinry

sin

sin

rdtdrx

cos

cos

rdtdry

xr

dtdrx

2

2 cos

cos

Page 37: X2 T07 04 uniform circular motion (2010)

y

x

P

r

cosrx

sinry

cosrx sinry

sin

sin

rdtdrx

cos

cos

rdtdry

xr

dtdrx

2

2 cos

cos

yr

dtdry

2

2 sin

sin

Page 38: X2 T07 04 uniform circular motion (2010)

y

x

P

r

cosrx

sinry

cosrx sinry

sin

sin

rdtdrx

cos

cos

rdtdry

xr

dtdrx

2

2 cos

cos

yr

dtdry

2

2 sin

sin

y

x

Page 39: X2 T07 04 uniform circular motion (2010)

y

x

P

r

cosrx

sinry

cosrx sinry

sin

sin

rdtdrx

cos

cos

rdtdry

xr

dtdrx

2

2 cos

cos

yr

dtdry

2

2 sin

sin

y

x

a

Page 40: X2 T07 04 uniform circular motion (2010)

y

x

P

r

cosrx

sinry

cosrx sinry

sin

sin

rdtdrx

cos

cos

rdtdry

xr

dtdrx

2

2 cos

cos

yr

dtdry

2

2 sin

sin

y

x

a

222 yxa

Page 41: X2 T07 04 uniform circular motion (2010)

y

x

P

r

cosrx

sinry

cosrx sinry

sin

sin

rdtdrx

cos

cos

rdtdry

xr

dtdrx

2

2 cos

cos

yr

dtdry

2

2 sin

sin

y

x

a

222 yxa

24

224

2424

ryx

yx

Page 42: X2 T07 04 uniform circular motion (2010)

y

x

P

r

cosrx

sinry

cosrx sinry

sin

sin

rdtdrx

cos

cos

rdtdry

xr

dtdrx

2

2 cos

cos

yr

dtdry

2

2 sin

sin

y

x

a

222 yxa

24

224

2424

ryx

yx

2ra

Page 43: X2 T07 04 uniform circular motion (2010)

y

x

P

r

cosrx

sinry

cosrx sinry

sin

sin

rdtdrx

cos

cos

rdtdry

xr

dtdrx

2

2 cos

cos

yr

dtdry

2

2 sin

sin

y

x

a

222 yxa

24

224

2424

ryx

yx

2ra

2mrFmaF

Page 44: X2 T07 04 uniform circular motion (2010)

y

x

P

r

cosrx

sinry

cosrx sinry

sin

sin

rdtdrx

cos

cos

rdtdry

xr

dtdrx

2

2 cos

cos

yr

dtdry

2

2 sin

sin

y

x

a

222 yxa

24

224

2424

ryx

yx

2ra

2mrFmaF

xy1tan

Page 45: X2 T07 04 uniform circular motion (2010)

y

x

P

r

cosrx

sinry

cosrx sinry

sin

sin

rdtdrx

cos

cos

rdtdry

xr

dtdrx

2

2 cos

cos

yr

dtdry

2

2 sin

sin

y

x

a

222 yxa

24

224

2424

ryx

yx

2ra

2mrFmaF

xy1tan

xy

xy

1

2

21

tan

tan

Page 46: X2 T07 04 uniform circular motion (2010)

y

x

P

r

cosrx

sinry

cosrx sinry

sin

sin

rdtdrx

cos

cos

rdtdry

xr

dtdrx

2

2 cos

cos

yr

dtdry

2

2 sin

sin

y

x

a

222 yxa

24

224

2424

ryx

yx

2ra

2mrFmaF

xy1tan

xy

xy

1

2

21

tan

tan

centrethes toward acting,, force a is There 2mrF

Page 47: X2 T07 04 uniform circular motion (2010)

b) A telecommunications satellite, of mass m, orbits Earth with constant angular velocity at a distance r

from the centre of the Earth.

The gravitational force exerted by Earth on the satellite is where

A

is a constant. By considering all other forces on the satellite to be negligible, show that;

2rAm

32

Ar

Page 48: X2 T07 04 uniform circular motion (2010)

b) A telecommunications satellite, of mass m, orbits Earth with constant angular velocity at a distance r

from the centre of the Earth.

The gravitational force exerted by Earth on the satellite is where

A

is a constant. By considering all other forces on the satellite to be negligible, show that;

2rAm

32

Ar

Page 49: X2 T07 04 uniform circular motion (2010)

b) A telecommunications satellite, of mass m, orbits Earth with constant angular velocity at a distance r

from the centre of the Earth.

The gravitational force exerted by Earth on the satellite is where

A

is a constant. By considering all other forces on the satellite to be negligible, show that;

2rAm

32

Ar

2mrxm

Page 50: X2 T07 04 uniform circular motion (2010)

b) A telecommunications satellite, of mass m, orbits Earth with constant angular velocity at a distance r

from the centre of the Earth.

The gravitational force exerted by Earth on the satellite is where

A

is a constant. By considering all other forces on the satellite to be negligible, show that;

2rAm

32

Ar

2mrxm 2r

Am

Page 51: X2 T07 04 uniform circular motion (2010)

b) A telecommunications satellite, of mass m, orbits Earth with constant angular velocity at a distance r

from the centre of the Earth.

The gravitational force exerted by Earth on the satellite is where

A

is a constant. By considering all other forces on the satellite to be negligible, show that;

2rAm

32

Ar

22

rAmmr

2mrxm 2r

Am

Page 52: X2 T07 04 uniform circular motion (2010)

b) A telecommunications satellite, of mass m, orbits Earth with constant angular velocity at a distance r

from the centre of the Earth.

The gravitational force exerted by Earth on the satellite is where

A

is a constant. By considering all other forces on the satellite to be negligible, show that;

2rAm

32

Ar

22

rAmmr

2

23

A

mAmr

2mrxm 2r

Am

Page 53: X2 T07 04 uniform circular motion (2010)

b) A telecommunications satellite, of mass m, orbits Earth with constant angular velocity at a distance r

from the centre of the Earth.

The gravitational force exerted by Earth on the satellite is where

A

is a constant. By considering all other forces on the satellite to be negligible, show that;

2rAm

32

Ar

22

rAmmr

2

23

A

mAmr

32

Ar

2mrxm 2r

Am

Page 54: X2 T07 04 uniform circular motion (2010)

(ii) A string is 50cm long and it will break if a ,mass exceeding 40kg is hung from it.A mass of 2kg is attached to one end of the string and it is revolved in a circle.Find the greatest angular velocity which may be imparted without breaking the string.

Page 55: X2 T07 04 uniform circular motion (2010)

(ii) A string is 50cm long and it will break if a ,mass exceeding 40kg is hung from it.A mass of 2kg is attached to one end of the string and it is revolved in a circle.Find the greatest angular velocity which may be imparted without breaking the string.

Page 56: X2 T07 04 uniform circular motion (2010)

(ii) A string is 50cm long and it will break if a ,mass exceeding 40kg is hung from it.A mass of 2kg is attached to one end of the string and it is revolved in a circle.Find the greatest angular velocity which may be imparted without breaking the string.

xm

Page 57: X2 T07 04 uniform circular motion (2010)

(ii) A string is 50cm long and it will break if a ,mass exceeding 40kg is hung from it.A mass of 2kg is attached to one end of the string and it is revolved in a circle.Find the greatest angular velocity which may be imparted without breaking the string.

xm mg

Page 58: X2 T07 04 uniform circular motion (2010)

(ii) A string is 50cm long and it will break if a ,mass exceeding 40kg is hung from it.A mass of 2kg is attached to one end of the string and it is revolved in a circle.Find the greatest angular velocity which may be imparted without breaking the string.

xm mg

T

Page 59: X2 T07 04 uniform circular motion (2010)

(ii) A string is 50cm long and it will break if a ,mass exceeding 40kg is hung from it.A mass of 2kg is attached to one end of the string and it is revolved in a circle.Find the greatest angular velocity which may be imparted without breaking the string.

xm mg

Tmgxm

T

Page 60: X2 T07 04 uniform circular motion (2010)

(ii) A string is 50cm long and it will break if a ,mass exceeding 40kg is hung from it.A mass of 2kg is attached to one end of the string and it is revolved in a circle.Find the greatest angular velocity which may be imparted without breaking the string.

xm mg

Tmgxm

T Tmg 0

Page 61: X2 T07 04 uniform circular motion (2010)

(ii) A string is 50cm long and it will break if a ,mass exceeding 40kg is hung from it.A mass of 2kg is attached to one end of the string and it is revolved in a circle.Find the greatest angular velocity which may be imparted without breaking the string.

xm mg

Tmgxm

N

T392

8.940

T Tmg 0

Page 62: X2 T07 04 uniform circular motion (2010)

(ii) A string is 50cm long and it will break if a ,mass exceeding 40kg is hung from it.A mass of 2kg is attached to one end of the string and it is revolved in a circle.Find the greatest angular velocity which may be imparted without breaking the string.

xm mg

Tmgxm

N

T392

8.940

T Tmg 0

Page 63: X2 T07 04 uniform circular motion (2010)

(ii) A string is 50cm long and it will break if a ,mass exceeding 40kg is hung from it.A mass of 2kg is attached to one end of the string and it is revolved in a circle.Find the greatest angular velocity which may be imparted without breaking the string.

xm mg

Tmgxm

N

T392

8.940

T Tmg 0

xm

Page 64: X2 T07 04 uniform circular motion (2010)

(ii) A string is 50cm long and it will break if a ,mass exceeding 40kg is hung from it.A mass of 2kg is attached to one end of the string and it is revolved in a circle.Find the greatest angular velocity which may be imparted without breaking the string.

xm mg

Tmgxm

N

T392

8.940

T Tmg 0

xm

T

Page 65: X2 T07 04 uniform circular motion (2010)

(ii) A string is 50cm long and it will break if a ,mass exceeding 40kg is hung from it.A mass of 2kg is attached to one end of the string and it is revolved in a circle.Find the greatest angular velocity which may be imparted without breaking the string.

xm mg

Tmgxm

N

T392

8.940

2mrT T Tmg 0

xm

T

Page 66: X2 T07 04 uniform circular motion (2010)

(ii) A string is 50cm long and it will break if a ,mass exceeding 40kg is hung from it.A mass of 2kg is attached to one end of the string and it is revolved in a circle.Find the greatest angular velocity which may be imparted without breaking the string.

xm mg

Tmgxm

N

T392

8.940

2mrT

25.02392 T Tmg 0

xm

T

Page 67: X2 T07 04 uniform circular motion (2010)

(ii) A string is 50cm long and it will break if a ,mass exceeding 40kg is hung from it.A mass of 2kg is attached to one end of the string and it is revolved in a circle.Find the greatest angular velocity which may be imparted without breaking the string.

xm mg

Tmgxm

N

T392

8.940

2mrT

25.02392

rad/s982392

3922

T Tmg 0

xm

T

Page 68: X2 T07 04 uniform circular motion (2010)

(ii) A string is 50cm long and it will break if a ,mass exceeding 40kg is hung from it.A mass of 2kg is attached to one end of the string and it is revolved in a circle.Find the greatest angular velocity which may be imparted without breaking the string.

xm mg

Tmgxm

N

T392

8.940

2mrT

25.02392

rad/s982392

3922

Exercise 9B; all

T Tmg 0

xm

T