Circular Motion Flashcards

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1
Q

Radian θ

A

The angle sub tended from an arc that has a length equal to the radius

  • θ = s/r
  • unit = radians
    (if s=r then θ = 1 radian)
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2
Q

Radians in a full circle

A

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3
Q

Linear Speed (v)

A
  • The distance travelled along the arc with respect to time

- v = s/t

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4
Q

Angular Velocity (w)

A
  • The rate of change of the angle with respect to time
  • w = θ/t
  • unit = rad/sec
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5
Q

Periodic Time (T)

A
  • The time taken for one complete revolution of the circle
  • T= 2πr/v
  • T = 2π/w
  • unit = seconds
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6
Q

Derivation of linear speed in terms of angular velocity

v = wr

A
1) θ = s/r 
 divide by t 
2) θ/t = s/rt 
sine  w = θ/t 
3)  w = s/rt
since v = s/t 
4) w = v/r 
5) v = wr 

(θ = angle in rads, r = radius in m)

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7
Q

Centripetal Force

A
  • the force directed towards the centre of a circle that is required to maintain circular motion
    (to keep a body moving in a circular path)
  • mass x centripetal acceleration
  • directed to centre so ⟂ to particle
  • F = mv²/r
  • F = mrw² (because a = v²/r and a = rw²)
    (e. g tension on string)
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8
Q

Force - ⟂

A
  • force applied ⟂ to a particle causes it to turn in a circle
  • force directed to centre will be ⟂ to particle
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9
Q

Centripetal acceleration

A

the acceleration towards the centre of a circle that holds a body in a circular orbit

  • a = v²/r
  • a = rw²
  • since particle is constantly moving in a circle
  • constantly changing direction
  • constantly changing velocity
  • constantly accelerating
    (speed always the same)
    (if acceleration is always towards centre there must be a force holding it there)
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10
Q

Derivation of centripetal acceleration in terms of angular velocity a = rw²

A
1) a = v²/r 
since v = rw 
2) a = (rw)²/r 
multiply out brackets
3) a = r²w²/r
divide by r 
4) a = rw²
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11
Q

Derivation of formulae for centripetal force

- F = mv²/r

A

1) F = ma
since a = v²/r
2) F = mv²/r

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12
Q

Derivation of formulae for centripetal force

- F = mrw²

A

1) F = ma
since a = rw²
2) F = mrw²

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13
Q

Satelites and Planetary Orbits - V ∝ √mass of the central body

A

centripetal force (mvr²) = gravitational force

1) mv²/r = GMm/r²
2) mv² = GMm/r
3) v² = GM/r
4) V = √GM/r

  • (r+h)
  • independent of mass of smaller object
  • speed and height linked
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14
Q

Derivation of T² = 4π²r²/GM

A
centripetal force (mrw²) = gravitational force 
1) mrw² = GMm/r²
2) w² = GM/r^3
since T = 2π/w ---- w = 2π/T
3) (2π/T)² = GM/r
4) 4π²/T² = GM/r 
5) T² = 4π²r²/GM

!!!! r = ( r + h )!!!
!!! unit = seconds!!!!

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15
Q

Kelper’s 1st law

A

planet’s move in elliptical orbits around the sun

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16
Q

Kelper’s second law

A

the line joining a planet and the sun sweeps out equal areas during equal intervals of time

17
Q

Kelper’s third law

A
  • T² ∝ r^3

- the square of the period of a planet orbit is proportional to the cube of the radius of it

18
Q

Different planets

A
  • g1/g2 = m1 x r2²/ m2 x r1²
  • g = GM/r²
    (G = newton’s gravitational constant)
    (g = gravity)
19
Q

Geostationary Orbits

A
  • stays at same point above earth
  • allows it to be found for telecommunication purposes
  • height important as determines speed
  • must travel at same periodic time as earth (24 hrs)

Must :

  • be on equatorial plane
  • period = 24 hours (24 x 60 x 60 seconds)
  • earth and satellite rotating in the same direction
20
Q

GPS satellites

A
  • not stationary
  • don’t stay at same point above earth
  • T is not 24 hours