Circular Motion: Angular Variables
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Transcript of Circular Motion: Angular Variables
R. Field 2/5/2013 University of Florida
PHY 2053 Page 1
Circular Motion: Angular Variables
The arc length s is related to the angle (in radians = rad) as follows:
• Arc Length:
rs r
s
if • Angular Displacement and Angular Velocity:
rdt
dsvv tt
dt
d
tt
0
lim
• Tangential Velocity and Angular Velocity:
(radians/second)
• Period and Frequency (constant ):
(360o = 2 rad)
TvrC t 2 22
tv
rT
Tf
1
(revolutions/second)
Tangential Velocityrvt
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Circular Motion: Radial Acceleration
Centripetal acceleration = “toward the center”
rvv tt ˆ)(
• Radial (centripetal) Acceleration:
rrrvrt
vt
va tt
t
tradial ˆ)(ˆ)(ˆ)(lim 2
0
r
vraa
t
radialradial
22 Magnitude = (vt)2/r
Direction = toward the center of the circle
Radial Acceleration
r̂
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Example Problem
• A puck of mass m slides in a circle of radius r = 0.5 m on a frictionless table while attached to a hanging cylinder of mass M = 2m by a cord through a hole in the table. What speed of the mass m keeps the cylinder at rest?
Answer: smm
Mgrv /13.3
Solution:
Mg
FT
FT
0 MgFT
r
vmmaF radialT
2
Mgr
vm
2
smmsm
grm
mgr
m
Mgrv
/13.3)5.0)(/8.9(2
22
2
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Example: Conical Pendulum
g
LTperiod
cos
22
2sin mrmamaT radialx
0cos ymamgT
x-component:
y-component:
• A stone of mass m is connected to a cord with length L and negligible mass. The stone is undergoing uniform circular motion in the horizontal plane. If the cord makes an angle with the vertical direction, what is the period of the circular motion?
cosL
g
g
L
g
r 22 )sin(tan
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Exam 1 Spring 2012: Problem 20
• A conical pendulum is constructed from a stone of mass M connected to a cord with length L and negligible mass. The stone is undergoing uniform circular motion in the horizontal plane as shown in the figure. If the cord makes an angle = 30o with the vertical direction and the period of the circular motion is 4 s, what is the length L of the cord (in meters)?Answer: 4.59 % Right: 34%
Rg
vR
vMMaF
MgF
xT
T
2
2
tan
sin
0cos
L
RT
Rv
v
RT
sin
4
2
2
222
L
M
L
Mg
x-axis
y-axis
R
FT
sin
4
tan
4tan
2
2
2
2
RL
gTR
gT
R
mssmgT
L 59.4)30cos(4
)4)(/8.9(
cos4 2
22
2
2
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Example Problem: Unbanked Curves
R
vtangential aradial
• A car of mass M is traveling in a circle with radius R on a flat highway with speed v. If the static coefficient of friction between the tires and the road is s, what is the maximum speed of the car such that it will not slide?
x-axis fs
N
R
y-axis
R
vMMaMaf radialxs
2
0 yMaMgN
gRMgM
RN
M
Rf
M
Rv ssss )()()( max
2max
Nfs s
gRv smax
x-component:
y-component:
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Exam 2 Spring 2011: Problem 4
• Near the surface of the Earth, a car is traveling at a constant speed v around a flat circular race track with a radius of 50 m. If the coefficients of kinetic and static friction between the car’s tires and the road are k = 0.1, s = 0.4, respectively, what is the maximum speed the car can travel without slipping?Answer: 14 m/s% Right: 74%
x-axis fs
FN
R
y-axis
R
vMMaMaf radialxs
2
0 yN MaMgF
gRMgM
RF
M
Rf
M
Rv ssNss )()()( max
2max
NsFfs
smmsmgRv s /14)50)(/8.9)(4.0( 2max
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Example Problem: Banked Curves
R
vMMaNf radials
2
sincos
0sincos ys MaMgfN
sincos s
MgN
x-component:
y-component:
)tan1(
)tan(
)sin(cos
)sincos(
)sincos(sincos)( max2max
s
s
s
s
ss
RgRg
NM
RNf
M
Rv
)tan1(
)tan(max
s
sRgv
• If the car in the previous problem is traveling on a banked road (angle ), what is the maximum speed of the car such that it will not slide?
Mg
Nf ss max)(
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Rolling Without Slipping: Rotation & Translation
R
v
s x-axis
x
• If a cylinder of radius R rolls without slipping along the x-axis then:
rsx
R
dt
dR
dt
dxv
Translational Speed
Rotational Speed