lecture equivalent system [compatibility mode]
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System of Forces: Reduction to a Force and Couple
A system of forces may be replaced by a collection of force-couple systems
acting at a given point O
The force and couple vectors may be combined into a
resultant force vector and a resultant couple vector,
CFrMFRR
O
The force-couple system at O may be moved to O
with the addition of the moment ofR about O ,
RsMMR
O
R
O
'
Engineers Mechanics- Equivalent Force-Couple System
bodyrigidtheinpresentanyifmomentcoupleappliedadd ,,
Further Reduction of a Force System to a wrench
Engineers Mechanics- Equivalent Force-Couple System
The pushing-turning action associated with
The tightening of a screw illustrates
collinear lines of action of the force and
couple vector that constitute a wrench
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Further Reduction of a System of Forces
If the resultant force and couple at O are mutually
perpendicular, they can be replaced by a single force actingalong a new line of action.
The resultant force-couple system for a system of forces
will be mutually perpendicular if:
1) the forces are coplanar, or
2) the forces are parallel.
Engineers Mechanics- Equivalent Force-Couple System
coplanar
parallel
Reduction of a Coplanar Force System to a Single Force
System can be reduced to a single forceby moving the line of action of until
its moment about Obecomes RO
M
R
In terms of rectangular coordinates,
R
Oxy MyRxR
Engineers Mechanics- Equivalent Force-Couple System
System of coplanar forces is reduced to a
force-couple system that is
mutually perpendicular.
R
OMR
and
FrMFR RO
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Example of a Coplanar Force System
Engineers Mechanics- Equivalent Force-Couple System
3 tugboats moving USS John F. Kennedy
Example of a Coplanar Force System
Equivalent Force Systems
Four tugboats are used to bring a ship to its pier.
Each tugboat exerts 100kN push in the direction
shown. Determinethepoint on hull (body) where a
single, more powerful tugboat should push to
produce the same effect as the original four
tugboats. Also determine the total push and its
directionto beexertedbythesingletugboat.
o
Solution Key:
Find the resultant force
and moment about O
Find the line of action
of resultant force
Find its intersectionwith the (hull) body of
the ship
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R = ( -100j ) + ( 0.8i - 0.6 j ) 100 + ( -100j ) + ( 0.6i + 0.8j ) 100
= T1 + T2 + T3 + T4= 100 ( 1.4i 1.8j ) kN
Equivalent Force Systems
Example of a Coplanar Force System
MoR= ri x Fi
= [ ( -100 x 24 ) + ( -100 x 0.6 x 144 - 100 x 0.8 x 24 ) + ( -100 x 224 )
+ ( 100 x 0.8 x184 + 100 x 0.6 x 24 ) ]= - 19200k kNm
SOLUTION
Y
XO
Prob.1
Equivalent Force SystemsExample of a Coplanar Force System
Equation of hull:y = (24/64)x & y = 24.
XO
Y
Try with y = (24/64)x
x = 19200/(180+140*24/64)
= 82.58 m > 64 m
x-intercept y-intercept
y = 24
(64, 24)
Y
X
Y
X
(0, 137.14)
(106.67, 0)
o
o
88
o
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Reduction of a Parallel Force System to a Single Force
Engineers Mechanics- Equivalent Force-Couple System
X
Y
Z
X
Y
Z
X
Y
Z
O
G
In other words:Use
appropriate
signs
A concrete foundation mat in the shape
of a regular hexagon with 3-m sides
supports four column loads as shown.
Determine the magnitude and the point
of application of the resultant four
loads.
Equivalent Force Systems
SOLUTION KEY
o Determine the magnitudeof the
equivalent force by just adding the
loads.
o Do the same for z axis, get x
co-ordinate.
o Equate the moment about the x axis
for the individual forces with that of
the equivalent force, get z co-ordinate.
Example of a Coplanar Force System
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: A C D E F F F F F R
80 kN 40 kN 100 kN 60 kN R j j j j
280 kN j
:x A A C C D D E E GM F z F z F z F z R z
GZkN28060sinm3kN60
80 kN 0 40 kN 3 m sin 60 60 kN 0
0.185577 mGZ
:z A A C C D D E E GM F x F x F x F x R x
80 kN 3 m cos 60 1.5 m 40 kN 1.5 m 60 kN 1.5 m
Equivalent Force Systems
100 kN 3 m cos60 1.5 m 280 kN Gx
Example of a Coplanar Force System
Distributed Force-Reduction to a Single Force
A distributed load is represented by plotting the load
per unit length, w (N/m) . The total load is equal tothe area under the load curve.
AdAdxwW
L
0
wdxxdWxWx A distributed load can be replaced by a concentratedload with a magnitude equal to the area under the
load curve and a line of action passing through the
area centroid.
Engineers Mechanics- Equivalent Force-Couple System
dAxAx
Total load (resultant)
Line of action
or
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Prob.3
Find the simplest resultant
for the forces acting on the
simply supported beam .
Equivalent Force Systems
SOLUTION KEY
o Get the equivalent concentrated
load of the distribute loading.
O X
10 N/m
300 N-m
30N/m
3m 3m 3m 3m
100 N
M
Example:
simply supported steel beam for
which self weight is acting as
u.d.l.
o Do the moment balance of all
external forces and moments
about o.
Example of Distributed Force
Prob.3
Distributed load :
R1 = ( 10 x 12 ) + ( ) ( 6 ) ( 20 )
= 180 N
= 7.33 m
SOLUTION
O
300 N-m
20N/m
3m 3m 3m 3m
6 m
10 m
10N/m
100 N
100N
180N
300 N-m
3m7.33m
4.714m
280N
Equivalent Force SystemsExample of Distributed Force
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1 -17
Water
Y
X
Z
Dam
xddx
x
Engineers Mechanics- Equivalent Force-Couple System
R
An automatic valve consists
of a 225 x 225 mm square
plate of uniform thickness
weighing 200 N (total). The
valve is pivoted about a
horizontal axis through A
located at a distance h = 100
mm above the lower edge.
Determine the depth of waterd for which the valve will
open.
b = 225mm
s=225mm
h = 100mm
d
Engineers Mechanics- Equivalent Force-Couple System
Example of Hydrostatic Pressure
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Prob.4
o Calculate the total moment (M) of the thrust about the bottom edge of the plate.
SOLUTION KEY
R
o At the verge of
opening the valve, the
centre of pressure
(C.O.P. ) of the
hydrostatic thrust will
pass through hinge
A.
d
b = 225
o Find the C.O.P when water level is at the top edge of the plate.
o Decide whether the required water level (d) is below/up of the plate top edge.
o Calculate the total hydrostatic force (R) on the plate for the depth of water d.
Engineers Mechanics- Equivalent Force-Couple System
Example of Hydrostatic Pressure
Prob.4
SOLUTION
Rx
b = 225
dx
R
d
b = 225 mm
x
h = 100mm
Engineers Mechanics- Equivalent Force-Couple System
Example of a Hydrostatic Pressure
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Prob.4
Rx
b = 225
dx
For any depth > 450 mm the C.O.P. will shift above hinge A and valve will open.
For d < 450 mm, the reaction at B prevents valve opening.
Have:M = h*R
For valve opening:
=h=100
Engineers Mechanics- Equivalent Force-Couple System
Example of Hydrostatic Pressure
1 -22
Redo the problem after
replacing the square plate
with an isosceles triangle
of width 225 mm at the top
and height of 225 mm.
SOLUTION KEY
The steps are same to the previous problem.
Find the C.O.P when the water level is at
the top edge of the plate:
SOLUTION
R
225mmx
b
Equivalent Force Systems
225 mm
225 mm
dx
Example of Hydrostatic Pressure
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Prob.5
R225mmx
b
225 mm
dx
*Note: for parabolic line loading the position of C.G. is L/2 (in this case 225/2)
Engineers Mechanics- Equivalent Force-Couple System
Example of Hydrostatic Pressure
Prob.5
225mm
xb=xR
At the verge of opening the valve, the centre of pressure (C.O.P. ) of the
hydrostatic thrust will pass through the hinge A.
Engineers Mechanics- Equivalent Force-Couple System
Example of Hydrostatic Pressure