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Physics of Bridges

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Title: Physics of Bridges


1
Physics of Bridges
  • Norman Kwong
  • Physics 409D

2
Forces
  • Before we take a look at bridges, we must first
    understand what are forces.
  • So, what is a force?
  • A force is a push or a pull
  • How can we describe forces?
  • Lets a take a look at Newtons law

3
Newtons Laws
  • Sir Isaac Newton helped create the three laws of
    motion
  • Newtons First law
  • When the sum of the forces acting on a particle
    is zero, its velocity is constant. In
    particular, if the particle is initially
    stationary, it will remain stationary.
  • an object at rest will stay at rest unless acted
    upon

4
Newtons Laws Continued
  • Newtons Second law
  • A net force on an object will accelerate itthat
    is, change its velocity. The acceleration will be
    proportional to the magnitude of the force and in
    the same direction as the force. The
    proportionality constant is the mass, m, of the
    object.
  • F mass acceleration

5
Newtons Laws Continued
  • Newtons Third law
  • The forces exerted by two particles on each other
    are equal in magnitude and opposite in direction
  • for every action, there is an equal and opposite
    reaction

6
So what do the laws tell us?
  • Looking at the second law we get Newtons famous
    equation for force Fma m is equal to the mass
    of the object and a is the acceleration
  • Units of force are Newtons
  • A Newton is the force required to give a mass of
    one kilogram and acceleration of one metre per
    second squared (1N1 kg m/s2)

7
So what do the laws tell us?
  • However, a person standing still is still being
    accelerated
  • Gravity is an acceleration that constantly acts
    on you
  • Fmg where g is the acceleration due to gravity

8
So what do the laws tell us?
  • Looking at the third law of motion
  • for every action, there is a equal and opposite
    reaction
  • So what does this mean?
  • Consider the following diagram
  • A box with a force due to gravity

9
So what do the laws tell us?
  • for every action, there is an equal and opposite
    reaction
  • A force is being exerted on the ground from the
    weight of the box. Therefore the ground must
    also be exerting a force on the box equal to the
    weight of the box
  • Called the normal force or FN

10
So what do the laws tell us?
  • From the first law
  • An object at rest will stay at rest unless acted
    upon
  • This means that the sums of all the forces but be
    zero.
  • Lets look back at our diagram

11
The idea of equilibrium
  • The object is stationary, therefore all the
    forces must add up to zero
  • Forces in the vertical direction FN and Fg
  • There are no horizontal forces

12
The idea of equilibrium
  • But FN is equal to Fg (from Newtons third law)
  • Adding up the forces we get FN Fg Fg Fg
    0
  • The object is said to be in equilibrium when the
    sums of the forces are equal to zero

13
Equilibrium
  • Another important aspect of being in equilibrium
    is that the sum of torques must be zero
  • What is a torque?
  • A torque is the measure of a force's tendency to
    produce torsion and rotation about an axis.
  • A torque is defined as tDF where D is the
    perpendicular distance to the force F.
  • A rotation point must also be chosen as well.

14
Torques
  • Torques cause an object to rotate
  • We evaluate torque by which torques cause the
    object to rotate clockwise or counter clockwise
    around the chosen rotation point

15
But what if the force isnt straight?
  • In all the previous diagrams, the forces have all
    been perfectly straight or they have all been
    perpendicular to the object.
  • But what if the force was at an angle?

16
Forces at an Angle
  • If the force is at an angle, we can think of the
    force as a triangle, with the force being the
    hypotenuse

17
Forces at an Angle
  • To get the vertical component of the force, we
    need to use trigonometry (also known as the
    x-component)
  • The red portion is the vertical part of the
    angled force (also known as the y-component
  • Tis the angle between the force and its
    horizontal part

18
  • To calculate the vertical part we take the sin of
    the force
  • Fvertical F sin (T)
  • Lets do a quick sample calculation
  • Assume T60o and F600N
  • Fvertical 600N sin (60o) 519.62N

19
Forces at an Angle
  • Like wise, we can do the calculation of the
    horizontal (the blue) portion by taking the
    cosine of the angle
  • Fhorizontal F cos (T)
  • Fhorizontal 600N cos (60o) 300N

20
Bridges
  • Now that we have a rough understanding of forces,
    we can try and relate them to the bridge.
  • A bridge has a deck, and supports
  • Supports are what holds the bridge up
  • Forces exerted on a support are called reactions
  • Loads are the forces acting on the bridge

21
Bridges
  • A bridge is held up by the reactions exerted by
    its supports and the loads are the forces exerted
    by the weight of the object plus the bridge
    itself.

22
Beam Bridge
  • Consider the following bridge
  • The beam bridge
  • One of the simplest bridges

23
What are the forces acting on a beam bridge?
  • So what are the forces?
  • There is the weight of the bridge
  • The reaction from the supports

24
Forces on a beam bridge
  • Here the red represents the weight of the bridge
    and the blue represents the reaction of the
    supports
  • Assuming the weight is in the center, then the
    supports will each have the same reaction

25
Forces on a beam bridge
  • Lets try to add the forces
  • Horizontal forces (x-direction) there are none
  • Vertical forces (y-direction) the force from the
    supports and the weight of the bridge

26
Forces on a beam bridge
  • Lets assume the bridge has a weight of 600N.
  • From the sums of forces Fy -600N 2 Fsupport0
  • Doing the calculation, the supports each exert a
    force of 300N

27
  • To meet the other condition of equilibrium, we
    look at the torques (tDF) with the red point
    being our rotation point
  • t (1m)(600N)-(2m)(600N)(3m)(600N) 0

28
Limitations
  • With all bridges, there is only a certain weight
    or load that the bridge can support
  • This is due to the materials and the way the
    forces are acted upon the bridge

29
What is happening?
  • There are 2 more other forces to consider in a
    bridge.
  • Compression forces and Tension forces.
  • Compression is a force that acts to compress or
    shorten the thing it is acting on
  • Tension is a force that acts to expand or
    lengthen the thing it is acting on

30
  • There is compression at the top of the bridge and
    there is tension at the bottom of the bridge
  • The top portion ends up being shorter and the
    lower portion longer
  • A stiffer material will resist these forces and
    thus can support larger loads

31
Bridge Jargon
  • Buckling is what happens to a bridge when the
    compression forces overcome the bridges ability
    to handle compression. (crushing of a pop can)
  • Snapping is what happens to a bridge when the
    tension forces overcome the bridges ability to
    handle tension. (breaking of a rubber band)
  • Span is the length of the bridge

32
How can deal with these new forces?
  • If we were to dissipate the forces out, no one
    spot has to bear the brunt of the concentrated
    force.
  • In addition we can transfer the force from an
    area of weakness to an area of strength, or an
    area that is capable of handling the force

33
A natural form of dissipation
  • The arch bridge is one of the most natural
    bridges.
  • It is also the best example of dissipation

34
  • In a arch bridge, everything is under compression
  • It is the compression that actually holds the
    bridge up
  • In the picture below you can see how the
    compression is being dissipated all the way to
    the end of the bridge where eventually all the
    force gets transferred to the ground

35
Compression in a Arch
  • Here is another look at the compression
  • The blue arrow here represents the weight of the
    section of the arch, as well as the weight above
  • The red arrows represent the compression

36
Arches
  • Here is one more look at the compression lines of
    an arch

37
A Stronger Bridge
  • Another way to increase the strength of a bridge
    is to add trusses
  • What are trusses??
  • A truss is a rigid framework designed to support
    a structure
  • How does a truss help the bridge?
  • A truss adds rigidity to the beam, therefore,
    increasing its ability to dissipate the
    compression and tension forces

38
So what does a truss look like?
  • A truss is essentially a triangular structure.
  • Consider the following bridge (Silver Bridge,
    South Alouette River, Pitt Meadows BC )

39
Trusses
  • We can clearly see the triangular structure built
    on top of a basic beam bridge.
  • But how does the truss increase the ability to
    handle forces?
  • Remember a truss adds rigidity to the beam,
    therefore, increasing its ability to dissipate
    the compression and tension forces

40
Trusses
  • Lets take a look at a simple truss and how the
    forces are spread out

41
  • Lets take a look at the forces here
  • Assumptions all the triangles are equal lateral
    triangles, the angle between the sides is 60o

42
  • Lets see how the forces are spread out

43
  • Sum of torques (1m)(-400N)
    (3m)(-800N)(4m)E0
  • E700N
  • Sum of forces AY E - 400N - 800N
  • Ay500N

44
  • Now that we know how the forces are laid out,
    lets take a look at what is happening at point A
  • Remember that all forces are in equilibrium, so
    they must add up to zero

45
  • Sum of FxTAC TAB cos 60o 0
  • Sum of FyTAB sin 60o 500N 0
  • Solving for the two above equations we get
  • TAB -577N TAC 289N

46
Compression and Tension
  • TAB -577N
  • TAC 289N
  • The negative force means that there is a
    compression force and a positive force means that
    there is a tension force

47
  • Lets take a look at point B

48
  • Sum of Fx TBD TBC cos 60o 577 cos 60o 0
  • Sum of Fy -400N 577sin60o TBCsin60o0
  • Once again, solving the two equations
  • TBC115N TBD-346N

49
Tension and Compression
  • TBC115N
  • TBD-346N
  • The negative force means that there is a
    compression force and a positive force means that
    there is a tension force

50
Forces in a Truss
  • If we calculated the rest of the forces acting on
    the various points of our truss, we will see that
    there is a mixture of both compression and
    tension forces and that these forces are spread
    out across the truss

51
Limitations of a Truss
  • As we can see from our demo, the truss can easily
    hold up weights, but there is a limitation.
  • Truss bridges are very heavy due to the massive
    amount of material involved in its construction.

52
Limitations of a Truss
  • In order to holder larger loads, the trusses need
    to be larger, but that would mean the bridge gets
    heavier
  • Eventually the bridge would be so heavy, that
    most of the truss work is used to hold the bridge
    up instead of the load

53
Suspension Bridge
  • Due to the limitations of the truss bridge type,
    another bridge type is needed for long spans
  • A suspension bridge can withstand long spans as
    well as a fairly decent load.

54
How Suspension Bridge Works
  • A suspension bridge uses the tension of cables to
    hold up a load. The cables are kept under
    tension with the use of anchorages that are held
    firmly to the Earth.

55
Suspension Bridge
  • The deck is suspended from the cables and the
    compression forces from the weight of the deck
    are transferred the towers. Because the towers
    are firmly in the Earth, the force gets
    dissipated into the ground.

56
Suspension Bridge
  • The supporting cables that are connected to the
    anchorages experience tension forces. The cables
    stretch due to the weight of the bridge as well
    as the load it carries.

57
Anchorages
  • Each supporting cable is actually many smaller
    cables bound together
  • At the anchorage points, the main cable separates
    into its smaller cables
  • The tension from the main cable gets dispersed to
    the smaller cables
  • Finally the tensional forces are dissipated into
    the ground via the anchorage

58
Suspension Bridge Cable
  • Here is a cross section picture of what a main
    cable of a suspension bridge looks like

59
A Variation on the Suspension
  • A cable stayed bridge is a variation of the
    suspension bridge.
  • Like the suspension bridge, the cable stayed
    bridge uses cables to hold the bridge and loads up

60
Comparison
61
Forces in a Cable Stayed
  • A cable stayed bridge uses the cable to hold up
    the deck
  • The tension forces in the cable are transferred
    to the towers where the tension forces become
    compression forces

62
Forces in a Cable Stayed
  • Lets take a quick look at the forces at one of
    the cable points.

63
Forces in a Cable Stayed
  • The Lifting force holds up the bridge
  • The higher the angle that the cable is attached
    to the deck, the more load it can withstand, but
    that would require a higher tower, so there has
    to be some compromise

64
Limitations
  • With all cable type bridges, the cables must be
    kept from corrosion
  • If the bridge wants to be longer, in most cases
    the towers must also be higher, this can be
    dangerous in construction as well during windy
    conditions
  • The bridge is only as good as the cable
  • If the cables snap, the bridge fails
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