4.9 Centripetal Acceleration

• An object moving in uniform circular motion travels with a constant angular velocity and angular speed
• However, its direction is always changing
  • Therefore, its linear velocity changes, so it must be accelerating
  • This is called a centripetal acceleration

• An object in circular motion is thus always accelerating
• This acceleration is called 'centripetal' because it is directed toward the centre of orbit

• To derive an equation for the magnitude of centripetal acceleration, consider an object in uniform circular motion between point A and B on a circle, as shown below: 

An object in uniform circular motion is accelerating toward the centre of orbit, O. Between A and B, the horizontal component of motion changes from v sinθ to –v sinθ

• At A and B, by resolving the horizontal and vertical components of linear velocity v, it can be seen that:
  • Initial vertical component of v = final vertical component of v which is v cosθ 
  • Initial horizontal component of v is v sinθ
  • Final horizontal component of v is –v sinθ

• This means the acceleration of the object is only horizontal, given by:

• Recalling the equations for angular velocity ω = θ /t and v = rω, then:

• The object's angular displacement is actually 2θ, therefore, the time t is given by 
• Therefore, substituting this into the equation for acceleration gives: 

• This equation is the acceleration of the object between points A and B
  • To find the instantaneous acceleration at an exact point on the circle, say point C, reduce the size of the angular displacement θ so it becomes infinitesimally small
  • This is shown in the image below: 

By taking the limit of angular displacement as zero, we can derive an equation for the instantaneous centripetal acceleration of the object at point C

• In the limit θ → 0 radians
  • The value of sin θ is approximately equal to θ
  • Therefore, (for very small angles)
  • This is known as the small angle approximation

• Therefore, the instantaneous acceleration is the centripetal acceleration:

• Where:
  • a = centripetal acceleration (m s^–2)
  • v = linear velocity (m s^–1)
  • r = radius of orbit (m)
  • ω = angular velocity (rad s^-1)

• The negative sign indicates that the centripetal acceleration is directed toward the centre of orbit 

• Centripetal acceleration is defined as:

The acceleration of an object towards the centre of a circle when an object is in motion (rotating) around a circle at a constant speed

• Its magnitude is calculated using the radius r and linear speed v:

• Using the equation relating angular speed ω and linear speed v:

 v = r⍵

• These equations can be combined to give another form of the centripetal acceleration equation:

• This equation shows that centripetal acceleration is equal to the radius times the square of the angular speed
• Alternatively, rearrange for r:

• This equation can be combined with the first one to give us another form of the centripetal acceleration equation:

• This equation shows how the centripetal acceleration relates to the linear speed and the angular speed

Centripetal acceleration is always directed toward the centre of the circle, and is perpendicular to the object’s velocity

• Where:
  • a = centripetal acceleration (m s⁻²)
  • v = linear speed (m s⁻¹)
  • ⍵ = angular speed (rad s⁻¹)
  • r = radius of the orbit (m)