Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel...
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Transcript of Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel...
![Page 1: Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel moving at constant speed. 1a) At what point is the.](https://reader035.fdocuments.in/reader035/viewer/2022062423/5697bfbf1a28abf838ca3324/html5/thumbnails/1.jpg)
Lecture 17: Torque & Rotational Equilibrium
![Page 2: Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel moving at constant speed. 1a) At what point is the.](https://reader035.fdocuments.in/reader035/viewer/2022062423/5697bfbf1a28abf838ca3324/html5/thumbnails/2.jpg)
Questions of YesterdayYou are riding on a Ferris wheel moving at constant speed. 1a) At what point is the net force acting on you the greatest?
a) the top b) the bottom
c) halfway between top and bottomd) the force is the same over the whole motion
1b) Is the net force doing work on you?a) YESb) NO
2) If the mass of the moon were doubled, what would happen to its centripetal acceleration?
a) it would increaseb) it would decreasec) it would stay the same
![Page 3: Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel moving at constant speed. 1a) At what point is the.](https://reader035.fdocuments.in/reader035/viewer/2022062423/5697bfbf1a28abf838ca3324/html5/thumbnails/3.jpg)
Force & Angular Acceleration
F = ma
What causes an object to accelerate?
Can an object be accelerating if there is no net force acting on the object?
What causes ANGULAR acceleration?
Force is needed to change the rate of rotation of an object
Is that all?
=t aT=r
![Page 4: Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel moving at constant speed. 1a) At what point is the.](https://reader035.fdocuments.in/reader035/viewer/2022062423/5697bfbf1a28abf838ca3324/html5/thumbnails/4.jpg)
F
F
FFF
ANGLE of force with respect to the radial direction affects angular acceleration
r r
POSITION of force with respect to the axis of rotation affects angular acceleration
Force & Angular Acceleration
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F
F
FFF
The rate of rotation of an object can’t change unless a FORCE is applied at a certain ANGLE and at a
DISTANCE from the axis of rotation
r r
Force & Angular Acceleration
![Page 6: Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel moving at constant speed. 1a) At what point is the.](https://reader035.fdocuments.in/reader035/viewer/2022062423/5697bfbf1a28abf838ca3324/html5/thumbnails/6.jpg)
r
Torque
FT
Fr
= ?F
The rate of rotation of an object can’t change unless a NET FORCE is applied at a certain ANGLE and at a
DISTANCE from the axis of rotation
The rate of rotation of an object can’t change unless the object is acted on by a net TORQUE ()
sinFr
= r*Fsin
Torque
Distance from axis of rotation
Force actingon object
Angle between forceand displacement from axis of rotation
F
![Page 7: Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel moving at constant speed. 1a) At what point is the.](https://reader035.fdocuments.in/reader035/viewer/2022062423/5697bfbf1a28abf838ca3324/html5/thumbnails/7.jpg)
F F
F
Direction of Force Vector F
r r
Torque Direction
+
-+
Direction of displacement vector r pointing FROM axis of rotation TO applied force
Direction of Rotation depends on
![Page 8: Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel moving at constant speed. 1a) At what point is the.](https://reader035.fdocuments.in/reader035/viewer/2022062423/5697bfbf1a28abf838ca3324/html5/thumbnails/8.jpg)
F F
F
Torque is a VECTOR!!Direction tells you direction of rotation
+ = Counterclockwise Motion- = Clockwise Motion
r r
Torque Direction
+
-+
![Page 9: Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel moving at constant speed. 1a) At what point is the.](https://reader035.fdocuments.in/reader035/viewer/2022062423/5697bfbf1a28abf838ca3324/html5/thumbnails/9.jpg)
Right-Hand Rule
Curl your FINGERS of your RIGHT hand in direction of
MOTION
THUMB points in direction of TORQUE Vector
CCW (+) Motion -> Torque = OUT of PAGE
CW (-) Motion -> Torque = INTO PAGE
TORQUE Direction is PERPENDICULAR to plane formed by
FORCE and DISPLACEMENT Vectors
F F
F
r r
+
+ -
![Page 10: Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel moving at constant speed. 1a) At what point is the.](https://reader035.fdocuments.in/reader035/viewer/2022062423/5697bfbf1a28abf838ca3324/html5/thumbnails/10.jpg)
Right-Hand Rule
TORQUE Direction is PERPENDICULAR to plane formed by
FORCE and DISPLACEMENT Vectors
F F
F
r r
If you have a FORCE acting on an object and a specific AXIS of rotation…
What is the direction of the TORQUE?
1) POINT the fingers of your right
hand in the direction of r
2) CURL your fingers in direction of F
3) THUMB points in direction of
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Torque
Does the seesaw rotate?
What is the TORQUE on the seesaw plank from each person?
What is the NET torque on the seesaw plank?
r r
Fg Fg
What is the net Force on the seesaw plank?
FPmass = m mass = m
Fgs
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Torque
r r
Fg Fg
FPmass = m mass = m
Force of gravity of a HOMOGENEOUS, SYMMETRIC body acts at the center of the object
Fgs
What is the TORQUE on the seesaw plank from each person?
What is the NET torque on the seesaw plank?
![Page 13: Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel moving at constant speed. 1a) At what point is the.](https://reader035.fdocuments.in/reader035/viewer/2022062423/5697bfbf1a28abf838ca3324/html5/thumbnails/13.jpg)
Equilibrium ConditionsAn object at rest or moving at constant linear velocity
and/or angular velocity (rotation) is in equilibrium
r r
Fg Fg
FPmass = m mass = m
Equilibrium (a = 0, = 0)
conditions
F = 0 = 0
Fgs
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Equilibrium ConditionsIs the system in equilibrium?
r/2 r
FgFg
FPmass = m mass = m
Equilibrium (a = 0, = 0)
conditions
F = 0 = 0
Fgs
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Equilibrium Conditions
rr
FgFg
FPmass = m mass = m
Is the system in equilibrium now?
Fgs
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Equilibrium Conditions
FgFg
mass = m mass = m
Is the system in equilibrium now?
rS
= + Fgr - Fgr + Fgsrs
Fgs
rr
FP
![Page 17: Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel moving at constant speed. 1a) At what point is the.](https://reader035.fdocuments.in/reader035/viewer/2022062423/5697bfbf1a28abf838ca3324/html5/thumbnails/17.jpg)
Equilibrium Conditions
Is there a point where the pivot could be placed to make the system in equilibrium?
FgFg
mass = m mass = m
Is the system in equilibrium now?
r3
= + Fgr1 - Fgr2 + Fgsr3 = 0
Fgs
r2r1
FP
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Choosing your Axis of Rotation
If we chose a different axis of rotation to calculate our net torque…would the system still be in equilibrium?
FgFg
mass = m mass = m
Do the torques exerted on the object depend on the chosen axis of rotation? What about the net torque?
r3Fgs
r2r1
FP
![Page 19: Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel moving at constant speed. 1a) At what point is the.](https://reader035.fdocuments.in/reader035/viewer/2022062423/5697bfbf1a28abf838ca3324/html5/thumbnails/19.jpg)
Choosing your Axis of Rotation
If we chose a different axis of rotation to calculate our net torque…would the system still be in equilibrium?
FgFg
mass = m mass = m
Do the torques exerted on the object depend on the chosen axis of rotation? What about the net torque?
r3 Fgs
r2r1
FP
axis ofrotation
![Page 20: Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel moving at constant speed. 1a) At what point is the.](https://reader035.fdocuments.in/reader035/viewer/2022062423/5697bfbf1a28abf838ca3324/html5/thumbnails/20.jpg)
Choosing your Axis of Rotation
FgFg
mass = m mass = m
r3 Fgs
r2r1
FP
axis ofrotation
The net torque of system is independent of the chosen axis of rotation…choose an axis that makes the problem
easiest!!
= +FPr1 - Fg (r1 + r2) - Fgsr3 = 0
![Page 21: Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel moving at constant speed. 1a) At what point is the.](https://reader035.fdocuments.in/reader035/viewer/2022062423/5697bfbf1a28abf838ca3324/html5/thumbnails/21.jpg)
Choosing your Axis of Rotation
The net torque of system is independent of the chosen axis of rotation…choose an axis that makes the problem
easiest!!
FgFg
mass = m mass = m
r3 Fgs
r2r1
FP
axis ofrotation
If there is an unknown force F, choose your axis to be at the position of that unknown force (r = 0 -> = 0)
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Choosing your Axis of Rotation
A uniform 10.0 N picture frame is supported as shown above.
Find the tension in the cords and the magnitude of F
F
T1T2
10.0 N
60o40.0 cm
30.0 cm
*
![Page 23: Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel moving at constant speed. 1a) At what point is the.](https://reader035.fdocuments.in/reader035/viewer/2022062423/5697bfbf1a28abf838ca3324/html5/thumbnails/23.jpg)
Center of Mass
r r
Fg Fg
FPmass = m mass = m
Force of gravity of a HOMOGENEOUS, SYMMETRIC body acts at the CENTER (the axis of symmetry) of the object
Fgs
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Center of Mass
r r
Fg Fg
FPmass = m mass = m
CENTER OF MASSThe point on an extended object where a single force Fg
= mg can act to represent the force of gravity acting on the entire extended object
Fgs
C.M.
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Center of Mass
r r
Fg Fg
FPmass = m mass = m
CENTER OF MASS
The rotation induced from Fg positioned at the center of
mass is the same as that induced from all the Fg’s
acting on the extended object
Fgs
C.M.
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Center of MassCENTER OF MASS of people + seesaw systemPosition of axis of rotation where system is in
equilibrium
FgFg
mass = m mass = m
rSFgs
r2r1
FP
C.M.
In 2-dimensions the center of mass is defined by an x and y coordinate (a single point in x-y space)
![Page 27: Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel moving at constant speed. 1a) At what point is the.](https://reader035.fdocuments.in/reader035/viewer/2022062423/5697bfbf1a28abf838ca3324/html5/thumbnails/27.jpg)
Center of Mass
FgFg
mass = m mass = m
rSFgs
r2r1
C.M.
xCM = m1x1 + m2x2 + m3x3….
m1 + m2 + m3….
m1y1 + m2y2 + m3y3….m1 + m2 + m3….
yCM =
=
=
∑mixi
∑mi
∑miyi
∑mi
![Page 28: Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel moving at constant speed. 1a) At what point is the.](https://reader035.fdocuments.in/reader035/viewer/2022062423/5697bfbf1a28abf838ca3324/html5/thumbnails/28.jpg)
Practice ProblemA 20.0-m, 500-N uniform ladder rest against a
frictionless wall, making an angle of 60.0o with the horizontal.
Find the horizontal and vertical forces exerted on the base of the ladder by the Earth when an 1000-N
firefighter is 5.0 m from the bottom.
If the ladder is just on the verge of slipping when the firefighter is 10.0 m up, what is the coefficient of static
friction between ladder and ground?
![Page 29: Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel moving at constant speed. 1a) At what point is the.](https://reader035.fdocuments.in/reader035/viewer/2022062423/5697bfbf1a28abf838ca3324/html5/thumbnails/29.jpg)
Practice ProblemA hungry 500-N bear walks out on a beam in an attempt to
retrieve some goodies (50 N) hanging at the end of the beam. The beam is attached to a wall by a hinge and supported from the other end by a cable. The beam is uniform, weighs 200 N
and is 10 m long.
-Draw a free-body diagram of the beam
-When the bear is at x = 1.00 m, find the tension in the wire and the
components of the reaction force at the hinge
-If the wire can withstand a maximum tension of 1000 N what is the maximum distance the bear can walk before the
wire breaks?
![Page 30: Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel moving at constant speed. 1a) At what point is the.](https://reader035.fdocuments.in/reader035/viewer/2022062423/5697bfbf1a28abf838ca3324/html5/thumbnails/30.jpg)
Questions of the Day1) If an object is rotating at a constant angular speed
which statement is true?a) the system is in equilibriumb) the net force on the object is ZEROc) the net torque on the object is ZEROd) all of the above
2) Student 1 (mass = m) sits on the left end of massless seesaw of length L and Student 2 (mass = 2m) sits at the right end. Where must the pivot be placed so the system is in equilibrium?a) L/2 b) L/3 from the right (from Student 2)c) L/3 from the left (from Student 1)d) the system cant be in equilibrium