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8 Rotational Dynamics
• describe/predict rotational behavior:
• motion, energy, momentum.
• with concepts of: rotational inertia & torque
• Homework:
• 30, 33, 39, 60, 65, 83, 89, 111.
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Translation and Rotation
• Translation: up, down, left, right, in, out
• Rotation:
• clockwise (cw),
• counterclockwise (ccw)
• //
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Rotational Dynamics: Newton’s 2nd Law for Rotation
inertia rotational
action rotationalnet
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Mass-Distribution Effect
Larger radius
Larger Speed
Larger Effort
Rotational Inertia ~ MR2
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Rotational Inertia ( I )
222
211 rmrmI
Example
22 )2)(5()3)(4( mkgmkgI
kg(m)2
2562036 mkg
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222
211 rmrmI
Example: Four identical masses. Axis passes symmetrically through center of mass.
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23
22
21 amamamamI
24maI
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222
211 rmrmI
2222 )2()2(00 amammmI 222 844 mamamaI
Example: Four identical masses. Axis passes through one end.
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You Try It
Calculate the Rotational Inertia of this system:
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Calculated Rot. Inertias, p.273
• rotational inertias of solid objects can be calculated
• need to know: a, b, c, d, e, g, h, j, k.
• omit: f, i
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Rotational Kinetic Energy
• Rotational K = ½(I)2.
• Example: Constant Power Source has 100kg, 20cm radius, solid disk rotating at 7000 rad/s.
• I = ½MR2 = ½(100kg)(0.2m)2 = 2kgm2.
• Rot K = ½ (2kgm2)(7000/s)2 = 49 MJ
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Torque () [N·m]
F
F
F
= lever-arm
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Torque Concept
• a small force can cause a large torque
• a large force can create no torque
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Rotationally Effective Application of Forces
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Rotationally Ineffective Application of Forces
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• torque = Fsin() (r)
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1. A pair of forces with equal magnitudes and opposite directions is acts as shown. Calculate the torque on the wrench.
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Example
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Rod is 3m Long.
40cos)3( m
NmmNF 5.11)3.2)(5(
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Newton’s 2nd Law (Rotation)
INet
maFNet
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Concept Review
• Torque: rotational action
• Rotational Inertia: resistance to change in rotational motion.
• Torque ~ force x lever-arm
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Equilibrium
• Translational: net-force = 0
• Rotational: net-torque = 0
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The drawing shows a person whose weight is 584N. Calculate the net force with which the floor pushes on each end of his body.
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Rotational Work-Energy Theorem
• (Work)rot = .
• Example: torque of 50 Nm is applied for one revolution.
• rotational work = (50Nm)(2rad) = 314 J
• (Rotational Work)net = Krot.
• Krot = ½I2.
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Angular Momentum (L)
• analog of translational momentum
• L = I [kgm2/s]
• Example: Disk R = 1m, M = 2kg, = 10/s
• I = ½MR2 = ½(1)(1)2 = 0.5
• L = I = (0.5kgm2)(10/s) = 5kgm2/s
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Conservation of Angular Momentum
• For an isolated system
• (I)before = (I)after
• Example: Stationary disk M,R is dropped on rotating disk M, R, i.
• (I)before = (I)after
• (½MR2)(i) = (½MR2 + ½MR2)(f)
• (f) = ½ (i)
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8 Summary
• All TRANSLATIONAL quantities;
• speed, velocity, acceleration,
• force, inertia, energy, and momentum,
• have ROTATIONAL analogs.
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Problem 33
• Pivot at left joint, Fj = ?, but torque = 0.
• ccw (Fm)sin15(18) = mg(26) = cw
• ccw (Fm)sin15(18) = (3)g(26) = cw
• (Fm) = (3)g(26)/sin15(18) = 160N
• Note: any point of arm can be considered the pivot (since arm is at rest)
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#39
• Left force = mg = 30g, Right = 25g
• mg = 30g + 25g m = 55kg
• ccw mg(xcg) = cw 30g(1.6)
• (55)g(xcg) = 30g(1.6)
• (55)(xcg) = 30(1.6)
• Xcg = (30/55)(1.6)
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#60, z-axis
• Each mass has r2 = 1.52 + 2.52.
• I = sum mr2 = (2+3+1+4)(1.52 + 2.52)
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#65
• First with no frictional torque, then with frictional torque as specified in problem.
• M = 0.2kg, R = 0.15m, m1 = 0.4, m2 = 0.8
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#83
• Pulley M, R. what torque causes it to reach ang. Speed. 25/s in 3rev?
• Alpha: use v-squared analog eqn.
• Torque = I = (½MR2)(
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#89, uniform sphere part
• Rolling at v = 5m/s, M = 2kg, R = 0.1m
• K-total = ½mv2 + ½I2.
• = ½(2)(5x5) + ½[(2/5)(2)(0.1x0.1)](5/0.1)2.
• = 25 + 10 = 35J
• Roll w/o slipping, no heat created, mech energy is conserved, goes all to Mgh.
• 35 = Mgh h = 35/Mg = 35(19.6) = 1.79m
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#111
• Ice skater, approximate isolated system
• Therefore:
• (I)before = (I)after
• (100)(i) = (92.5)(f)
• (f) = (100/92.5)(i)
• K-rot increases by this factor squared times new rot. Inertia x ½.
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Example: Thin rod formulas.
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K = Ktranslation + Krotation
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Angular Momentum• Symbol: L Unit: kg·m2/s
• L = mvr = m(r)r = mr2 = I.
• v is perpendicular to axis
• r is perpendicular distance from axis to line containing v.
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Angular Momentum• Symbol: L Unit: kg·m2/s
• L = mvr = m(r)r = mr2 = I.
• v is perpendicular to axis
• r is perpendicular distance from axis to line containing v.
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13) Consider a bus designed to obtain its motive power from a large rotating flywheel (1400. kg of diameter 1.5 m) that is periodically brought up to its maximum speed of 3600. rpm by an electric motor at the terminal. If the bus requires an average power of 12. kilowatts, how long will it operate between recharges?Answer: 39. minutesDiff: 2 Var: 1 Page Ref: Sec. 8.4
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6) A 82.0 kg painter stands on a long horizontal board 1.55 m from one end. The 15.5 kg board is 5.50 m long. The board is supported at each end.(a) What is the total force provided by both supports?(b) With what force does the support, closest to the painter, push upward?
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28) A 4.0 kg mass is hung from a string which is wrapped around a cylindrical pulley (a cylindrical shell). If the mass accelerates downward at 4.90 m/s2, what is the mass of the pulley?A) 10.0 kgB) 4.0 kgC) 8.0 kgD) 2.0 kgE) 6.0 kg
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19) A solid disk with diameter 2.00 meters and mass 4.0 kg freely rotates about a vertical axis at 36. rpm. A 0.50 kg hunk of bubblegum is dropped onto the disk and sticks to the disk at a distance d = 80. cm from the axis of rotation.(a) What was the moment of inertia before the gum fell?(b) What was the moment of inertia after the gum stuck?(c) What is the angular velocity after the gum fell onto the disk?
(a) 2.0 kg-m2(b) 2.3 kg-m2(c) 31. rpm
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3. The drawing shows the top view of two doors. The doors are uniform and identical. The mass of each door is M and width as shown below is L. How do their rotational accelerations compare?
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A Ring, a Solid-Disk, and a Solid-Sphere are released from rest from the top of an incline. Each has the same mass and radius. Which will reach the bottom first?
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5. The device shown below is spinning with rotational rate i when the movable rods are out. Each moveable rod has length L and mass M. The central rod is length 2L and mass 2M.
Calculate the factor by which the angular velocity is increased by pulling up the arms as
shown.
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How large is the height h in the drawing? The ball’s initial speed is 4.0 m/s. Does it depend on M and R?
solid ball rolls without slipping
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Rotational Review
rs
(angles in radians)
tavg
rvt
rat tavg
2rac
+ 4 kinematic equations
tc aaa
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Rotation Disk-Hanging Mass
0
500
1000
1500
2000
2500
0 200 400 600
mass (grams)
mt
an
d m
t2/1
0
mt
mt2
Graph showing mt2 is more constant than mt
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Angular Momentum Calculation
L = I
Example: Solid Disk M = 2kg R = 25cm
Spins about its center-of-mass at 35 rev/s
skgm
revradsrevmkgIL
/7.13
)/2)(/35()25)(.2(2
221
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4. A one-meter-stick has a mass of 480grams. a) Calculate its rotational inertia about an axis perpendicular to the stick and through one of its ends.b) Calculate its rotational inertia about an axis perpendicular to the stick and through its center-of-mass.c) Calculate its angular momentum if spinning on axis (b) at a rate of 57rad/s.
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Conservation of Angular Momentum
• Example: 50 grams of putty shot at 3m/s at end of 200 gram thin 80cm long rod free to rotate about its center.
• Li = mvr = (0.050kg)(3m/s)(0.4m)
• Lf = I = {(1/12)(0.200kg)(0.8m)2 + (0.050kg)(0.4m)2}()
• final rotational speed of rod&putty =
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tavg
tavg
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57
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