scee-271-12-sec-9
Transcript of scee-271-12-sec-9
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CEE 271: Applied Mechanics II, Dynamics
Lecture 5: Ch.12, Sec.9
Prof. Albert S. Kim
Civil and Environmental Engineering, University of Hawaii at Manoa
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ABSOLUTE DEPENDENT MOTION ANALYSIS OF
TWO PARTICLES
Todays objectives: Students
will be able to
1 Relate the positions,
velocities, and
accelerations of particlesundergoingdependent
motion.
In-class activities:
Reading Quiz
Applications
Define Dependent Motion
Develop Position, Velocity,
and Acceleration
Relationships
Concept Quiz
Group Problem Solving
Attention Quiz
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READING QUIZ
1 When particles are interconnected by a cable, the motionsof the particles are
(a) always independent.(b) always dependent.(c) not always dependent.
(d) None of the above.ANS:(b)
2 If the motion of one particle is dependent on that of anotherparticle, each coordinate axis system for the particles
(a) should be directed along the path of motion.
(b) can be directed anywhere.(c) should have the same origin.(d) None of the above.
ANS:(a)
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APPLICATIONS
The cable and pulley system
shown can be used to modify the
speed of the mine car,A, relativeto the speed of the motor,M.
It is important to establish therelationships between the various
motions in order to determine the
power requirementsfor the motor
and thetensionin the cable.
For instance, if the speed of the cable (P) is known(because we know the motor characteristics), how can we
determine the speed of the mine car? Will theslopeof the
track have any impact on the answer?
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APPLICATIONS(continued)
Rope and pulleyarrangements are
often used to assist in lifting
heavy objects. The total
lifting forcerequired from thetruck depends on both
the weight and the accelerationof
the cabinet.
How can we determine the
acceleration and velocity of thecabinet if the acceleration of the
truck isknown?
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DEPENDENT MOTION (Section 12.9)
In many kinematics problems, the
motion of one object willdependon
the motion of another object.
The blocks in this figure are
connected by aninextensiblecordwrapped around a pulley. If block Amoves downwardalong the inclined
plane, blockB will moveupthe otherincline.
The motion of each block can be related mathematically bydefining position coordinates,sA andsB. Each coordinateaxis is defined froma fixed pointordatum line, measured
positivealong each plane in thedirection of motionof each
block.
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DEPENDENT MOTION (continued)
In this example, position coordinates
sA andsB can be defined fromfixed datum linesextending from the
centerof the pulley along eachincline to blocksAandB .
If the cord has a fixed length, the
position coordinatessA andsB arerelated mathematically by
sA+lCD+sB =lT
werelTis the total cord length andlCD is the length of cordpassing over the arcCDon the pulley.
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DEPENDENT MOTION (continued)
The velocities of blocksA andB canbe related by differentiating the
position equation. Note thatlCD andlT remainconstant, so
dlCDdt
=dlTdt
= 0
dsAdt
+dsBdt
= 0 vB = vA
The negative sign indicates that asA moves down theincline (positivesAdirection),B moves up the incline(negativesB direction).
Accelerations can be found by differentiating the velocity
expression. Prove to yourself thataB = aA.
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DEPENDENT MOTION EXAMPLE
Consider a more complicated
example. Position coordinates (sAandsB) are defined from fixed
datum lines, measured along thedirection of motionof each block.
Note thatsB is only definedtothecenter of the pulley aboveblockB ,since this block moves with the
pulley. Also,h is aconstant.
The red colored segments of the cord remain constantin
length during motion of the blocks.
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DEPENDENT MOTION EXAMPLE (continued)
The position coordinates are related bythe equation
2sB+h+sA=lT
wherelTis the total cord length minusthe lengths of the red segments.
SincelT andh remainconstantduringthe motion, the velocities and
accelerations can be related by twosuccessive time derivatives:
2vB = vA and 2aB = aA When blockB movesdownward(+sB), blockAmoves to
theleft(sA). Remember to be consistent with your sign
convention!10/20
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DEPENDENT MOTION EXAMPLE (continued)
This example can also be worked
by defining the position
coordinate forB (sB) from thebottompulley instead of the top
pulley. The position, velocity, and
acceleration relations then
become
2(h sB) +h+sA=lTand 2vB =vA , 2aB =aA
Prove to yourself that the results are the same, even if the
sign conventions are different than the previous
formulation.
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DEPENDENT MOTION: PROCEDURES
These procedures can be used to relate the dependentmotion of particles moving along rectilinearpaths (only themagnitudesof velocity and acceleration change, not their
line of direction).1 Defineposition coordinatesfromfixed datum lines, along the
path of each particle. Different datum lines can be used foreach particle.
2 Relate the position coordinates to the cord length.Segments of cord that do notchange in length during themotion may be left out.
3 If a system contains more than one cord, relate the positionof a point on one cord to a point on another cord. Separateequations are writtenfor each cord.
4 Differentiatethe position coordinate equation(s) to relatevelocities and accelerations. Keep track of signs!
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EXAMPLE
Given: In the figure on the left, the cord
atAis pulled down with a speed of2 m/s.
Find: The speed of blockB .
Plan:1 There aretwocords involved in the
motion in this example.2 There will betwoposition equations
(one for each cord).3 Writethese two equations,combine
them, and thendifferentiatethem.
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EXAMPLE (continued)
Solution:
1 Define the position coordinates from a fixed datum line.
Three coordinates must be defined: one for pointA(sA),one for blockB (sB), and one for blockC(sC).
Define the datum line through the toppulleyD(which has afixedposition).
sAcan be definedtothe pointA.
sB can be defined tothe center of the
pulley aboveB. sC is definedtothe center of pulleyC.
All coordinates are defined as
positive downand along the direction of
motion of each point/object.
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EXAMPLE (continued)
2. Write position/length equations foreach cord. Definel1as the length of thefirst cord,minusany segments of
constant length. Definel2 in a similarmanner for the second cord:
Cord 1: sA+ 2sC=l1Cord 2: sB+ (sB sC) =l2
3. EliminatingsCbetween the twoequations, we get
sA+ 4sB =l1+ 2l24. Relate velocities by differentiating this expression. Note
thatl1 andl2 are constant lengths.vA+ 4vB = 0 vB = 0.25vA= 0.25(2) = 0.5 m/sThe velocity of blockB is 0.5 m/s up(negativesBdirection).
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CONCEPT QUIZ
1. Determine the speed of block B .(a) 1 m/s(b) 2 m/s(c) 4 m/s(d) None of the above.
ANS:(a)
2. Two blocks are interconnected by a cable.
Which of the following is correct ?(a) vA = vB(b) (vx)A = (vx)B(c) (vy)A = (vy)B(d) All of the above.
ANS:(d)
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GROUP PROBLEM SOLVING
Given: In this pulley system, block A ismoving downwardwith a speed of4 ft/swhile blockCis moving up at2 ft/s.
Find: The speed of blockB .
Plan:All blocks are connected to a single cable, so only one
position / length equationwill be required. Define position
coordinates for each block, write out the position relation,
and then differentiate it to relate the velocities.17/20
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GROUP PROBLEM SOLVING (continued)
Solution:
1. A datum line can be drawn through theupper, fixed pulleysand position
coordinates defined from this line to
each block (or the pulley above the
block).
2. DefiningsA,sB, andsCas shown, theposition relation can be written:
sA+ 2sB+sC=l
3. Differentiate to relate velocities:
vA+ 2vB+vC = 0
4 + 2vB+ (2) = 0
vB = 1 ft/s
The velocity of blockB is 1 ft/s up(negativesB direction). 18/20
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ATTENTION QUIZ
1 Determine the speed of blockB whenblockAis moving down at 6 ft/swhileblockCis moving down at 18 ft/s.
(a) 24ft/s(b) 3 ft/s
(c) 12ft/s(d) 9 ft/s
ANS:(c)
2 Determine the velocity vector of blockAwhen blockB is moving downward with
a speed of 10 m/s.(a) (8i+ 6j) m/s(b) (4i+ 3j) m/s(c) (8i 6j) m/s(d) (3i+ 4j) m/s
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note
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