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Tight Corners
Physics in Sport – Lesson 1
Learning intentions
 Explain why circular motion even at uniform speed is accelerated motion

 Use vector subtraction to show this
 Use formulas to solve problems
STARTER – give some examples of motion in a circle
 In which do you think the speed is uniform?
Measuring angles and arcs
 Circumference of a circle

s  2r
Where does this come from?
• Measuring angles in radians
• One radian is the angle

Angle in radians = length of arc
radius

s
 
r

s
2r
  
 2
r
r
• 360 degrees = 2π radians
Motion in a circle


If an object is moving in a circle what is it’s

a) Distance travelled

b) Displacement
c) Linear speed

•

2r
v
T

Theoretically what is it’s average velocity?
Why is it accelerated motion?
v1

 What is the definition of velocity?
 It is a vector quantity

 What is the definition of acceleration?
v4
v2

Q.
v3

 It is a vector quantity

In your own words explain using the definitions why
circular motion is accelerated motion
Why is it accelerated motion?
v1

 To find the change in velocity (Δv) we
need to subtract the velocity vectors.

v2

 v2-v1= v2+(-v1 )=Δv

v2

Δv Δv
-v1
Centripetal Acceleration
v1
v2
Δv

 To find the change in velocity any 2
short time intervals is always towards
the centre of the circle

v2
-v1

If the change in velocity is
towards the centre then so
is the acceleration
Centripetal Acceleration
 Acceleration is the rate of change of
velocity.

v1
v2
Δv
a= Δv
t

 It towards the centre of the circle.
 It is given by

2

v
a
r
Forces cause accelerations
 If there is such a thing as centripetal
acceleration then these must be
caused by forces (that’s what forces
do)

F  ma

2

v
a
r

 There are different centripetal forces

2

v
F m
r
Causes of Centripetal Force
Causes of Centripetal Force
Causes of Centripetal Force
Worked Example: Centripetal Force
A stone of mass 0.5 kg is swung round in a horizontal circle (on a frictionless surface) of radius
0.75 m with a steady speed of 4 m s-1.

 Calculate:
(a) the centripetal acceleration of the stone

acceleration = v2/r = 42 / 0.75 = 21.4 m s-2
(b) the centripetal force acting on the stone.

F = ma = mv2/r = [0.5 ´ 42] / 0.75 = 10.7 N
 Notice that this is a linear acceleration and not an angular acceleration. The angular velocity
of the stone is constant and so there is no angular acceleration.

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Physics of Circular Motion

  • 1. Tight Corners Physics in Sport – Lesson 1
  • 2. Learning intentions  Explain why circular motion even at uniform speed is accelerated motion  Use vector subtraction to show this  Use formulas to solve problems
  • 3.
  • 4. STARTER – give some examples of motion in a circle  In which do you think the speed is uniform?
  • 5. Measuring angles and arcs  Circumference of a circle s  2r Where does this come from? • Measuring angles in radians • One radian is the angle Angle in radians = length of arc radius s   r s 2r     2 r r • 360 degrees = 2π radians
  • 6. Motion in a circle  If an object is moving in a circle what is it’s a) Distance travelled b) Displacement c) Linear speed • 2r v T Theoretically what is it’s average velocity?
  • 7. Why is it accelerated motion? v1  What is the definition of velocity?  It is a vector quantity  What is the definition of acceleration? v4 v2 Q. v3  It is a vector quantity In your own words explain using the definitions why circular motion is accelerated motion
  • 8. Why is it accelerated motion? v1  To find the change in velocity (Δv) we need to subtract the velocity vectors. v2  v2-v1= v2+(-v1 )=Δv v2 Δv Δv -v1
  • 9. Centripetal Acceleration v1 v2 Δv  To find the change in velocity any 2 short time intervals is always towards the centre of the circle v2 -v1 If the change in velocity is towards the centre then so is the acceleration
  • 10. Centripetal Acceleration  Acceleration is the rate of change of velocity. v1 v2 Δv a= Δv t  It towards the centre of the circle.  It is given by 2 v a r
  • 11. Forces cause accelerations  If there is such a thing as centripetal acceleration then these must be caused by forces (that’s what forces do) F  ma 2 v a r  There are different centripetal forces 2 v F m r
  • 15. Worked Example: Centripetal Force A stone of mass 0.5 kg is swung round in a horizontal circle (on a frictionless surface) of radius 0.75 m with a steady speed of 4 m s-1.  Calculate: (a) the centripetal acceleration of the stone acceleration = v2/r = 42 / 0.75 = 21.4 m s-2 (b) the centripetal force acting on the stone. F = ma = mv2/r = [0.5 ´ 42] / 0.75 = 10.7 N  Notice that this is a linear acceleration and not an angular acceleration. The angular velocity of the stone is constant and so there is no angular acceleration.