chapter5a_torque.ppt
TRANSCRIPT
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Chapter 5A. Torque
A PowerPoint Presentation by
Paul E. Tippens, Professor of Physics
Southern Polytechnic State University
2007
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Torque is a twist
or turn that tendsto producerotation. * * *
Applications are
found in manycommon toolsaround the home
or industry whereit is necessary toturn, tighten orloosen devices.
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Objectives: After completing this
module, you should be able to: Define and give examples ofthe terms torque,
moment arm, axis, andline of action of a force.
Draw, label and calculate the moment armsfora variety of applied forces given an axis ofrotation.
Calculate the resultant torqueabout any axis
given the magnitude and locations of forces onan extended object.
Optional:Define and apply the vector crossproductto calculate torque.
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Definition of Torque
Torqueis defined as the tendency toproduce a change in rotational motion.
Examples:
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Torque is Determined by Three Factors:
The magnitudeof the applied force.
The directionof the applied force.
The locationof the applied force.
20 N
Magnitude of force
40 N
The 40-Nforce
produces twice thetorque as does the
20-Nforce.
Each of the 20-N
forces has a differenttorque due to the
direction of force. 20 N
Direction of Force
20 Nq
q20 N
20 N
Location of forceThe forces nearer the
end of the wrenchhave greater torques.
20 N
20 N
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Units for Torque
Torque is proportional to the magnitude ofF and to the distance r from the axis. Thus,a tentativeformula might be:
t= Fr Units: Nmor lbft
6cm
40 N
t= (40 N)(0.60 m)
= 24.0 Nm, cw
t= 24.0 Nm, cw
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Direction of Torque
Torque is a vector quantity that hasdirection as well as magnitude.
Turning the handle of ascrewdriver clockwiseand
then counterclockwisewilladvance the screw firstinward and then outward.
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Sign Convention for Torque
By convention, counterclockwise torques arepositive and clockwise torques are negative.
Positivetorque:Counter-clockwise,
out of page
cw
ccw
Negativetorque:clockwise, into page
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Line of Action of a Force
The line of actionof a force is an imaginaryline of indefinite length drawn along thedirection of the force.
F1
F2
F3Line ofaction
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The Moment Arm
The moment armof a force is the perpendiculardistance from the line of action of a force to theaxis of rotation.
F2
F1
F3
r
rr
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Calculating Torque
Read problem and draw a rough figure.
Extend line of action of the force.
Draw and label moment arm.
Calculate the moment arm if necessary.
Apply definition of torque:
t= Fr Torque = force x moment arm
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Example 1: An 80-Nforce acts at the end ofa 12-cmwrench as shown. Find the torque.
Extend line of action, draw, calculate r.
t= (80 N)(0.104 m)
= 8.31 N m
r = 12cm sin 600
= 10.4 cm
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Alternate: An 80-Nforce acts at the end ofa 12-cmwrench as shown. Find the torque.
Resolve 80-N force into components as shown.
Note from figure: rx = 0 and ry= 12 cm
t= (69.3 N)(0.12 m) t= 8.31 N m as before
positive
12 cm
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Calculating Resultant Torque
Read, draw, and label a rough figure.
Draw free-body diagram showing all forces,distances, and axis of rotation.
Extend lines of action for each force.
Calculate moment arms if necessary.
Calculate torques due to EACH individual forceaffixing proper sign. CCW (+) and CW (-).
Resultant torque is sum of individual torques.
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Example 2: Find resultant torque aboutaxisAfor the arrangement shown below:
300
300
6 m 2 m
4 m
20 N30 N
40 NA
Find t due to
each force.
Consider 20-N
force first:
r = (4 m) sin 300
= 2.00 m
t= Fr = (20 N)(2 m)
= 40 N m, cw
The torque about A isclockwise and negative.
t20= -40 N m
r
negative
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Example 2 (Cont.): Next we find torquedue to 30-Nforce about same axisA.
300
300
6 m 2 m
4 m
20 N30 N
40 NA
Find t due to
each force.
Consider 30-N
force next.
r = (8 m) sin 300
= 4.00 m
t= Fr = (30 N)(4 m)
= 120 N m, cw
The torque about A isclockwise and negative.
t30= -120N m
rnegative
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Example 2 (Cont.): Finally, we considerthe torque due to the 40-Nforce.
Find t due to
each force.
Consider 40-N
force next:
r = (2 m) sin 900
= 2.00 m
t= Fr = (40 N)(2 m)
= 80 N m, ccw
The torque about A isCCW and positive.
t40= +80N m
300
300
6 m 2 m
4 m
20 N30 N
40 NA
r
positive
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Example 2 (Conclusion): Find resultanttorque about axisAfor the arrangement
shown below:
300300
6 m 2 m4 m
20 N30 N
40 NA
Resultant torque
is the sum ofindividual torques.
tR= - 80N m Clockwise
tR=
t20 +
t20+
t20= -40 N m -120 N m + 80 N m
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Part II: Torque and the Cross
Product or Vector Product.Optional Discussion
This concludes the general treatmentof torque. Part II details the use ofthe vector product in calculating
resultant torque. Check with yourinstructor before studying this section.
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The Vector Product
Torque can also be found by using the vectorproduct of force Fand position vector r. Forexample, consider the figure below.
F
qr
F Sin qThe effect of the forceFat angle q(torque)
is to advance the boltoutof the page.
Torque
Magnitude:
(FSinq)r
Direction = Out of page (+).
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Definition of a Vector Product
The magnitude of the vector (cross) productof two vectorsAand Bis defined as follows:
AxB= l A l l B l Sin q
F xr = l F l l r l Sin q Magnitude only
F
(F Sinq) r or F (r Sinq)
In our example, the cross product of F and r is:
In effect, this becomes simply:q
r
F Sin
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Example: Find the magnitude of thecross product of the vectors r and Fdrawn below:
r xF = l r l l F l Sin q
r xF = (6 in.)(12 lb) Sin 600
r xF = l r l l F l Sin q
r xF= (6 in.)(12 lb) Sin 1200
Explain difference. Also, what about Fx r?
12 lb
r xF = 62.4 lb in.
Torque
600
6 in.
Torque600
6 in.
12 lb r xF = 62.4 lb in.
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Direction of the Vector Product.
The directionof avector product isdetermined by the
right hand rule. A
C
BB
-CA
A x B = C (up)
B x A = -C (Down)
Curl fingers of right handin direction of cross pro-duct (Ato B) or (BtoA).Thumbwill point in thedirection of product C.
What is directionof A x C?
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Example: What are the magnitude anddirection of the cross product, r x F?
r xF = l r l l F l Sin q
r xF = (6 in.)(10 lb) Sin 500
r xF = 38.3 lb in.
10 lbTorque
500
6 in. Magnitude
Out
r
FDirection by right hand rule:
Out of paper (thumb) or +k
r xF = (38.3 lb in.) k
What are magnitude and direction of F x r?
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Cross Products Using (i,j,k)
x
z
yConsider 3D axes (x, y, z)
Define unit vectors, i, j, kij
kConsider cross product: i x i
i x i= (1)(1) Sin 00
= 0
i
ij x j= (1)(1) Sin 00= 0
k x k = (1)(1)Sin 00= 0
Magnitudes arezero for parallelvector products.
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Vector Products Using (i,j,k)
Consider 3D axes (x, y, z)
Define unit vectors, i, j, kx
z
y
ij
k Consider dot product: i xj
i x j= (1)(1) Sin 900
= 1j x k= (1)(1) Sin 900= 1
k x i = (1)(1) Sin 900= 1
ji
Magnitudes are1for perpendicularvector products.
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Vector Product (Directions)
x
z
y
ij
k
i x j= (1)(1) Sin 900
= +1 kj x k= (1)(1) Sin 900= +1 i
k x i = (1)(1) Sin 900= +1j
Directions are given by theright hand rule. Rotatingfirst vector into second.
k
j
i
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Vector Products Practice (i,j,k)
x
z
y
ij
ki xk= ?
k xj = ?
Directions are given by theright hand rule. Rotatingfirst vector into second.
k
j
i 2ix -3 k= ?
- j (down)
- i (left)
+ 6j (up)
j x-i = ? + k (out)
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Using i,j Notation - Vector Products
Consider: A= 2 i- 4j and B= 3 i + 5j
A xB= (2 i - 4 j) x (3 i + 5 j) =
(2)(3) ixi + (2)(5) ixj + (-4)(3) jxi + (-4)(5) jxj
k -k0 0
A xB= (2)(5) k + (-4)(3)(-k) = +22 k
Alternative: A= 2 i- 4j
B= 3 i + 5j
A xB= 10 - (-12) = +22 k
Evaluatedeterminant
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Summary
Torqueis the product of a forceand itsmoment armas defined below:
The moment armof a force is the perpendicular distance
from the line of action of a force to the axis of rotation.
The line of actionof a force is an imaginary line ofindefinite length drawn along the direction of the force.
t= Fr Torque = force x moment arm
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Summary: Resultant Torque
Read, draw, and label a rough figure.
Draw free-body diagram showing all forces,distances, and axis of rotation.
Extend lines of action for each force.
Calculate moment arms if necessary.
Calculate torques due to EACH individual forceaffixing proper sign. CCW (+) and CW (-).
Resultant torque is sum of individual torques.
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CONCLUSION: Chapter 5A
Torque