Chapter 16 - Circular Motion Flashcards
define the radian
“A radian is the angle subtended by a circular arc with length equal to the radius of the circle”
what is the equation for the radian
Angle (radians) = arc length/radius
define angular velocity
“the angular velocity, (lowercase omega w), of an object moving in a circular path is defined as the rate of change of angle”
what are the three equations for angular velocity
w = delta theta/ time
w = 2(Pi)/T
(T is period)
w = 2f(Pi)
(f is frequency)
what are the units for angular velocity
radS^-1
usually
why is something moving in a circular path accelerating and what does this mean
- when moving on a circular path at a constant speed your velocity is still changing because the direction of travel changes and velocity is a vector
- this means there is an acceleration
- this means there must be a resultant force
what is the name of this resultant force acting when an object moves on a circular path
the centripetal force
what are the key features of the centripetal force
- it acts perpendicular to velocity
- it acts towards the centre of the circle
- it has no ‘horizontal’ component in the same direction as the object’s tangental speed so the speed of the object remains constant
how can we derive the equations for linear velocity and angular velocity
speed = distance/time
distance in this case = 2r(pi)
and time = T (period)
because it’s the circumference of the circle so
v = 2r(pi)/T
as w = 2(pi)/T this gives us
V = wr
what is the equation linking linear and angular velocity
v = wr
what is the derivation for the equation using acceleration and radius
- imagine a small section of a circle, radius r
- the angle is deltatheta, the arc length is delta(x), the velocity at one end of the arc is Va and Vb at the other
By definition delta(theta) = delta(x)/r
As Va and Vb act in different directions there must have been an acceleration, this is given by
a = delta(v)/delta(t)
as delta(x) is small, we can model it as a straight line so delta(x) = v x delta(t)
substituting gives
delta(theta) = vdelta(t)/r
as delta(theta) also = delta(v)/v
this means
vdelta(t)/r = delta(v)/v
so v^2/r = delta(v)/delta(r) = a (from part 1)
thus V^2/r = a
what are the two equations for acceleration on a circle
a = V^2/r
and
a = w^2 x r
how to derive the two centripetal force equations
- we know F = Ma
- we know a = V^2/r and a = (w^2)r
so therefore
F = mv^2/r
F = m(w^2)r
what are the three derivations you need to know
1) derivation of v = wr
2) derivation of a = V^2/r and a = w^2r
3) derivation of F = mv^2/r and F = mw^2r
what is an experiment we can do to investigate circular motion
- set up equipment where there is a mass on a string, passing through a metal/glass tube, attached to another mass
- the length of the string above the tube is r
- we know that the faster we swing the mass, the more likely the hanging mass is to rise up
- this is because swinging the mass faster means it requires a greater centripetal force, if the weight of the other mass isn’t sufficient then the weight will rise up due to tension in the string
- if the centripetal force required is lower than the weight of the hanging mass then the hanging mass will drop
- this along with our equations allows us to do a variety of experiments and plot different graphs