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Design of Springs
Topic 2
Kinds of Springs
Springs can be classified according to the direction and the nature of
the force exerted by the spring when it is deflected.
• Push
• Pull
• Radial
• Torsional
Helical compression springs are typically made from round wire,
wrapped into a straight, cylindrical form with a constant pitch between
adjacent coils.
End Configurations
Four practical end configurations are shown in Figure.
.
Helical Extension Spring
Helical extension springs appear to be similar to
compression springs, having a series of coils wrapped
into a cylindrical form.
However, in extension springs, the coils either touch
or are closely spaced under the no-load condition.
Then as the external tensile load is applied, the coils
separate.
Without an applied load, the spring's length is called the free length.
When a compression force is applied, the coils are pressed more
closely together until they all touch, at which time the length is the
minimum possible called the solid length.
Torsion Spring
Torsion Spring is used to exert a torque as the spring is deflected by
rotation about its axis. The common spring action clothespin uses a
torsion spring to provide the gripping action.
Leaf Spring
Leaf springs are made from one or more flat strips of brass, bronze,
steel, or other materials loaded as cantilevers or simple beams. They
can provide a push or a pull force as they are deflected from their free
condition. Large forces can be exerted within a small space by leaf
springs.
Helical Compression Springs
Helical compression springs are typically made from round wire,
wrapped into a straight, cylindrical form with a constant pitch between
adjacent coils.
In the most common form of helical compression spring, round wire is
wrapped into a cylindrical form with a constant pitch between adjacent
coils.
For medium- to large-size springs used in machinery, the squared and
ground-end treatment provides a flat surface on which to .seat the
spring. The end coil is collapsed against the adjacent coil (squared),
and the surface is ground until at least 270° of the last coil is in contact
with the bearing surface.
Applications of Helical Compression Springs
Springs made from smaller wire (less than approximately 0.50 mm)
are usually squared only, without grinding.
You are probably familiar with many uses of helical compression
springs. The retractable ballpoint pen depends on the helical
compression spring, usually installed around the ink supply barrel.
Suspension systems for cars, trucks, and motorcycles frequently
incorporate these springs. Other automotive applications include the
valve springs in engines, hood linkage counterbalancing, and the
clutch pressure-plate springs.
Spring Diameters
The wire diameter is d, the mean coil diameter is D.
The Outside Diameter DO and Inside Diameter DI
are of interest mainly to define the minimum hole
in which it will fit or the maximum pin over which
it can be placed.
𝐷𝑂 = 𝐷 + 𝑑
𝐷𝐼 = 𝐷 − 𝑑
The minimum recommended diametral clearances
between DO and a hole or between DI and a pin are
0.10D.
Spring Lengths
The free length Lf is the
length that the spring
assumes when it is exerting
no force, as if it were
simply sitting on a table.
It is important to understand the relationship between the length ofthe
spring and the force exerted by it
Spring Lengths
This is obviously the
shortest possible length that
the spring can have.
The spring is usually not
compressed to the solid
length during operation.
The solid length, Ls is found when the spring is collapsed to the point
where all coils are touching.
Spring Lengths
The shortest length for the spring during normal operation is the
operating length, LO. At times, a spring will be designed to operate
between two limits of deflecfion.
Consider the valve spring for an engine. When the valve is open, the
spring assumes its shortest length, which is LO. Then when the valve is
closed, the spring gets longer but still exerts a force to keep the valve
securely on its seat. The length at this condition is called the installed
length LI. So the valve spring length changes from LO to LI during
normal operation as the valve itself reciprocates.
Forces in Springs
We will use the symbol F to indicate forces exerted by a spring, with
various subscripts to specify which level of force is being considered.
The subscripts correspond to those used for the lengths. Thus,
• Fs = force at solid length, Ls: the maximum force that the spring ever sees.
• Fo = force at operating length, Ls: the maximum force the spring sees in
normal operation.
• Fi = force at installed length, Ls
• Ff = force at free length, Ls: this force is zero
Spring Rate
The relationship between the force exerted by a spring and its
deflection is called its spring rate, k.
Any change in force divided by the corresponding change in deflection
can be used to compute the spring rate:
𝑘 = ∆𝐹/∆𝐿
Spring Index
The ratio of the mean diameter of the spring to the wire diameter is
called the spring index. C:
𝐶 = 𝐷/𝑑
It is recommended that C be greater than 5.0, with typical machinery
springs having C values ranging from 5 to 12.
For C less than 5, the forming of the spring will be very difficult, and
the severe deformation required may create cracks in the wire. The
stresses and the deflections in springs are dependent on C. and a larger
C will help to eliminate the tendency for a spring to buckle.
Number of Coils
The total number of coils in a spring will be called N. But in the
calculation of stress and deflections for a spring, some of the coils are
inactive and are neglected.
For example, in a spring with squared and ground ends or simply
squared ends, each end coil is inactive, and the number of active coils,
Na is N — 2.
For plain ends, all coils are active: Na = N. For plain coils with ground
ends, Na — N - 1.
Pitch
Pitch, p refers to the axial distance from a point on one coil to the
corresponding point on the next adjacent coil.
The relationships among the pitch, free length, wire diameter, and
number of active coils are given as:
Installation Considerations
Frequently, a spring is installed in a cylindrical hole or around a rod.
When it is, adequate clearances must be provided.
When a compression spring is compressed, its diameter gets larger.
Thus, the inside diameter of a hole enclosing the spring must be
greater than the outside diameter of the spring to eliminate rubbing.
An initial diametral clearance of one-tenth of the wire diameter is
recommended for springs having a diameter of 0.50 in (12 mm) or
greater.
Installation Considerations
Frequently, a spring is installed in a cylindrical hole or around a rod.
When it is, adequate clearances must be provided.
When a compression spring is compressed, its diameter gets larger.
Thus, the inside diameter of a hole enclosing the spring must be
greater than the outside diameter of the spring to eliminate rubbing.
An initial diametral clearance of one-tenth of the wire diameter is
recommended for springs having a diameter of 0.50 in (12 mm) or
greater.
Materials Used for Springs
Virtually any elastic material can be used for a spring. However, most
mechanical applications use metallic wire—high-carbon steel (most
common), alloy steel, .stainless steel, brass, bronze, beryllium copper,
or nickel-base alloys.
Most spring materials are made according to specifications of the
ASTM.
Types of Loading and Allowable Stresses
The allowable stress to be used for a spring depends on the type of
loading, the material, and size of the wire. Loading is usually classified
into three types:
Light service: Static loads or up to 10 000 cycles of loading with a
low rate of loading (nonimpact).
• Average service: Typical machine design situations; moderate rate of
loading and up to 1 million cycles.
Severe service: Rapid cycling for above 1 million cycles; possibility
of shock or impact loading; engine valve .springs are a good example.
Stresses and Deflections for Helical Compression Spring
As a compression spring is compressed under an axial load, the wire is
twisted. Therefore, the stress developed in the wire is torsional shear
stress, and it can be derived from the classical equation
𝜏 = 𝑇𝑐/𝐽.
When the equation is applied specifically to a helical compression
spring, some modifying factors are needed to account for the curvature
of the spring wire and for the directshear stress created as the coils
resist the vertical load.
Also, it is convenient to express the shear stress in terms of the design
variables encountered in springs.
Stresses and Deflections for Helical Compression Spring
The resulting equation for stress is attributed to Wahl. The maximum shear
stress, which occurs at the inner surface of the wire, is
𝜏 =
8𝐾𝐹𝐷𝑚
𝜋𝐷𝑚
3 =
8𝐾𝐹𝐶
𝜋𝐷𝑤
2
These are two forms of the same equation as C = Dm/Dw.
Normally we will be concerned about the stress when the spring is
compressed to solid length under the influence of Fs and when the spring is
operating at its normal maximum load, Fo.
Notice that the stress is inversely proportional to the cube of the wire
diameter. This illustrates the great effect that variation in the wire size has
on the performance of the spring.
Stresses and Deflections for Helical Compression Spring
The Wahl factor, K. in Equation is the term that accounts for the
curvature of the wire and the direct shear stress. Analytically, K is
related to C:
𝐾 =
4𝐶 − 1
4𝑐 − 4
+
0.615
𝐶
Figure shows a plot of K versus C for round wire. Recall that C = 5 is
the recommended minimum value of C. The value of K rises rapidly
for C < 5.
Deflection
Because the primary manner of loading on the wire of a helical
compression spring is torsion, the deflection is computed from the
angle of twist formula:
𝜃 =
𝑇𝐿
𝐺𝐽
Where 𝜃 = angle of twist in radians
T = applied torque
L = length of the wire
G = modulus of elasticity of the material in shear
J = polar moment of inertia of the wire
Deflection
Because the primary manner of loading on the wire of a helical
compression spring is torsion, the deflection is computed from the
angle of twist formula:
𝜃 =
𝑇𝐿
𝐺𝐽
Where 𝜃 = angle of twist in radians
T = applied torque
L = length of the wire
G = modulus of elasticity of the material in shear
J = polar moment of inertia of the wire
Linear Deflection
For convenience, we will u.se a different form of the equation in order
to calculate the linear deflection, f of the spring from the typical design
variables of the spring. The resulting equation is
𝑓 =
8𝐹𝐷𝑚
3
𝑁𝑎
𝐺𝐷𝑤
4 =
8𝐹𝐶3
𝑁𝑎
𝐺𝐷𝑤
Buckling
The tendency for a spring to buckle increases as the
spring becomes tall and slender, much as for a column.
Figure shows plots of the critical ratio of deflection to
the free length versus the ratio of free length to the
mean diameter for the spring. Three different end
conditions are described in the figure.
As an example of the use of this figure, consider a
spring having squared and ground ends, a free length
of 6.0 in, and a mean diameter of 0.75 in. We want to
know what deflection would cause the spring to
buckle.
Buckling
First compute
𝐿𝑓
𝐷𝑚
=
6.0
0.75
= 8.0
from Figure, the
critical deflection
ratio is 0.20.
Buckling
From this we can
compute the critical
deflection:
That is, if the spring is
deflected more than
1.20 in, the spring
should buckle.
Analysis of Spring Characteristics
This section demonstrates the use of the concepts developed in
previous sections to analyze the geometry and the performance
characteristics of a given spring.
Assume that you have found a spring but there are no performance
data available for it. By making a few measurements and
computations, you should be able to determine those characteristics.
One piece of information you would have to know is the material
from which the spring is made so that you could evaluate the
acceptability of calculated stress levels.
Example Problem 1
A spring is known to be made from music wire, ASTM A228 steel, but
no other data are known. You are able to measure the following
features using simple measurement tools:
Free length = Lf = 1.75 in
Outside diameter = OD = 0.561 in
Wire diameter = Dw = 0.055 in
The ends are squared and ground.
The total number of coils is 10.0.
This spring will be used in an application where the normal operating
load is to be 14.0 lb. Approximately 300 000 cycles of loading are
expected.
Example Problem 1
For this spring, compute and/or do the following:
1. The music wire gage number, mean diameter, inside diameter, spring index, and
Wahl factor.
2. The expected stress at the operating load of 14.0 lb.
3. The deflection of the spring under the 14.0-lb load.
4. The operating length, solid length, and spring rate.
5. The force on the spring when it is at its solid length and the corresponding stress
at solid length.
6. The design stress for the material; then compare it with the actual operating
stress.
7. The maximum permissible stress; then compare it with the stress at solid length.
8. Check the spring for buckling and coil clearance.
9. Specify a suitable diameter for a hole in which to install the spring.
Example Problem 1
Example Problem 1
Example Problem 1
Example Problem 1
Example Problem 1
Design of Helical Compression Springs
The objective of the design of helical compression springs is to specify
the geometry for the spring to operate under specified limits of load
and deflection, possibly with space limitations, also.
We will specify the material and the type of service by considering the
environ ment and the application.
Example Problem 2
A helical compression spring is to exert a force of 8.0 lb when
compressed to a length of 1.75 in. At a length of 1.25 in, the force
must be 12.0 lb. The spring will be installed in a machine that cycles
slowly, and approximately 200 000 cycles total are expected. The
temperature will not exceed 200°F. The spring will be installed in a
hole having a diameter of 0.75 in.
For this application, specify a suitable material, wire diameter, mean
diameter, OD, ID, free length, solid length, number of coils, and type
of end condition. Check the stress at the maximum operating load and
at the solid length condition.
Example Problem 2 (Solution 1)
The procedure works directly toward the overall geometry of the
spring by specifying the mean diameter to meet the space limitations.
The process requires that the designer have tables of data available for
wire diameters and graphs of design stresses for the material from
which the spring will be made.
We must make an initial estimate for the design stress for the material
by consulting the charts of design stress versus wire diameter to make
a reasonable choice. In general, more than one trial must be made, but
the results of early trials will help you decide the values to use for later
trials.
Example Problem 2 (Solution 1)
Step 1: Specify a material and its shear modulus of elasticity, G.
For this problem, several standard spring materials can be used. Let's
select ASTM A231 chromium-vanadium steel wire, having a value of
G = 11 200 000 psi.
Step 2: From the problem statement, identify the operating force, Fo
the operating length at which that force must be exerted, Lo ; the force
at some other length, called the installed force, FI : and the installed
length. LI. Remember, Fo is the maximum force that the spring
experiences under normal operating conditions.
Example Problem 2 (Solution 1)
Many times, the second force level is not specified. In that ca.se, let FI
= 0, and specify a design value for the free length, LF in place of LI.
For this problem, FO= 12 lb; LO = 1.25in; FI = 8 lb; and LI = 1.75in.
Step 3: Compute the spring rate, k
𝑘 =
𝐹𝑂 − 𝐹𝐼
𝐿𝐼 − 𝐿𝑂
=
12 − 8
1.75 − 1.25
= 8𝑙𝑏/𝑖𝑛
Step 4: Compute the free length, L,
𝐿𝐹 = 𝐿𝐼 +
𝐹𝐼
𝑘
= 1.75 +
8
8
= 2.75𝑖𝑛
Example Problem 2 (Solution 1)
The second term in the preceding equation is the amount of deflection
from free length to the installed length in order to develop the installed
force, FI. Of course, this step becomes unnecessary if the free length is
specified in the original data.
Step 5: Specify an initial estimate for the mean diameter, Dm
Keep in mind that the mean diameter will be smaller than the OD and
larger than the ID. Judgment is necessary to get started.
For this problem, let's specify Dm = 0.60 in. This should permit the
installation into the 0.75-in-diameter hole.
Example Problem 2 (Solution 1)
Step 6: Specify an initial design stress.
The charts for the design stresses for the selected material can be
consulted, considering also the service. In this problem, we should use
average service. Then for the ASTM A231 steel, as shown in Figure, a
nominal design stress would be 130 000 psi. This is strictly an estimate
based on the strength of the material. The process includes a check on
stress later
Step 7: Compute the trial wire diameter. Notice that everything else in
the equation is known except the Wahl factor K, because it depends on
the wire diameter itself. But K varies only little over the normal range
of spring indexes, C. From Figure, note that K = 1.2 is a nominal
value. This, too, will be checked later.
Example Problem 2 (Solution 1)
Example Problem 2 (Solution 1)
With the assumed value of K, some simplification can be done:
Example Problem 2 (Solution 1)
Step 8: Select a standard wire diameter from the tables, and then determine
the design stress and the maximum allowable stress for the material at that
diameter.
The design stress will normally be for average service, unless high cycling
rates or shock indicate thatsevere service is warranted.
The light service curve should be used with care because it is very near to
the yield strength. In fact, we will use the light service curve as an estimate
of the maximum allowable stress.
For this problem, the next larger standard wire size is 0.0625 in, no. 16 on
the U.S. Steel Wire Gage chart. For this size, the curves in Figure for ASTM
A231 steel wire show the design stress to be approximately 145 000 psi for
average service, and the maximum allowable stress to be 170 000 psi from
the light service curve.
Example Problem 2 (Solution 1)
Example Problem 2 (Solution 1)
Example Problem 2 (Solution 1)
Example Problem 2 (Solution 1)

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02 Design of Springs.pptx

  • 2. Kinds of Springs Springs can be classified according to the direction and the nature of the force exerted by the spring when it is deflected. • Push • Pull • Radial • Torsional Helical compression springs are typically made from round wire, wrapped into a straight, cylindrical form with a constant pitch between adjacent coils.
  • 3. End Configurations Four practical end configurations are shown in Figure. .
  • 4. Helical Extension Spring Helical extension springs appear to be similar to compression springs, having a series of coils wrapped into a cylindrical form. However, in extension springs, the coils either touch or are closely spaced under the no-load condition. Then as the external tensile load is applied, the coils separate. Without an applied load, the spring's length is called the free length. When a compression force is applied, the coils are pressed more closely together until they all touch, at which time the length is the minimum possible called the solid length.
  • 5. Torsion Spring Torsion Spring is used to exert a torque as the spring is deflected by rotation about its axis. The common spring action clothespin uses a torsion spring to provide the gripping action.
  • 6. Leaf Spring Leaf springs are made from one or more flat strips of brass, bronze, steel, or other materials loaded as cantilevers or simple beams. They can provide a push or a pull force as they are deflected from their free condition. Large forces can be exerted within a small space by leaf springs.
  • 7. Helical Compression Springs Helical compression springs are typically made from round wire, wrapped into a straight, cylindrical form with a constant pitch between adjacent coils. In the most common form of helical compression spring, round wire is wrapped into a cylindrical form with a constant pitch between adjacent coils. For medium- to large-size springs used in machinery, the squared and ground-end treatment provides a flat surface on which to .seat the spring. The end coil is collapsed against the adjacent coil (squared), and the surface is ground until at least 270° of the last coil is in contact with the bearing surface.
  • 8. Applications of Helical Compression Springs Springs made from smaller wire (less than approximately 0.50 mm) are usually squared only, without grinding. You are probably familiar with many uses of helical compression springs. The retractable ballpoint pen depends on the helical compression spring, usually installed around the ink supply barrel. Suspension systems for cars, trucks, and motorcycles frequently incorporate these springs. Other automotive applications include the valve springs in engines, hood linkage counterbalancing, and the clutch pressure-plate springs.
  • 9. Spring Diameters The wire diameter is d, the mean coil diameter is D. The Outside Diameter DO and Inside Diameter DI are of interest mainly to define the minimum hole in which it will fit or the maximum pin over which it can be placed. 𝐷𝑂 = 𝐷 + 𝑑 𝐷𝐼 = 𝐷 − 𝑑 The minimum recommended diametral clearances between DO and a hole or between DI and a pin are 0.10D.
  • 10.
  • 11. Spring Lengths The free length Lf is the length that the spring assumes when it is exerting no force, as if it were simply sitting on a table. It is important to understand the relationship between the length ofthe spring and the force exerted by it
  • 12. Spring Lengths This is obviously the shortest possible length that the spring can have. The spring is usually not compressed to the solid length during operation. The solid length, Ls is found when the spring is collapsed to the point where all coils are touching.
  • 13. Spring Lengths The shortest length for the spring during normal operation is the operating length, LO. At times, a spring will be designed to operate between two limits of deflecfion. Consider the valve spring for an engine. When the valve is open, the spring assumes its shortest length, which is LO. Then when the valve is closed, the spring gets longer but still exerts a force to keep the valve securely on its seat. The length at this condition is called the installed length LI. So the valve spring length changes from LO to LI during normal operation as the valve itself reciprocates.
  • 14. Forces in Springs We will use the symbol F to indicate forces exerted by a spring, with various subscripts to specify which level of force is being considered. The subscripts correspond to those used for the lengths. Thus, • Fs = force at solid length, Ls: the maximum force that the spring ever sees. • Fo = force at operating length, Ls: the maximum force the spring sees in normal operation. • Fi = force at installed length, Ls • Ff = force at free length, Ls: this force is zero
  • 15. Spring Rate The relationship between the force exerted by a spring and its deflection is called its spring rate, k. Any change in force divided by the corresponding change in deflection can be used to compute the spring rate: 𝑘 = ∆𝐹/∆𝐿
  • 16. Spring Index The ratio of the mean diameter of the spring to the wire diameter is called the spring index. C: 𝐶 = 𝐷/𝑑 It is recommended that C be greater than 5.0, with typical machinery springs having C values ranging from 5 to 12. For C less than 5, the forming of the spring will be very difficult, and the severe deformation required may create cracks in the wire. The stresses and the deflections in springs are dependent on C. and a larger C will help to eliminate the tendency for a spring to buckle.
  • 17. Number of Coils The total number of coils in a spring will be called N. But in the calculation of stress and deflections for a spring, some of the coils are inactive and are neglected. For example, in a spring with squared and ground ends or simply squared ends, each end coil is inactive, and the number of active coils, Na is N — 2. For plain ends, all coils are active: Na = N. For plain coils with ground ends, Na — N - 1.
  • 18. Pitch Pitch, p refers to the axial distance from a point on one coil to the corresponding point on the next adjacent coil. The relationships among the pitch, free length, wire diameter, and number of active coils are given as:
  • 19. Installation Considerations Frequently, a spring is installed in a cylindrical hole or around a rod. When it is, adequate clearances must be provided. When a compression spring is compressed, its diameter gets larger. Thus, the inside diameter of a hole enclosing the spring must be greater than the outside diameter of the spring to eliminate rubbing. An initial diametral clearance of one-tenth of the wire diameter is recommended for springs having a diameter of 0.50 in (12 mm) or greater.
  • 20. Installation Considerations Frequently, a spring is installed in a cylindrical hole or around a rod. When it is, adequate clearances must be provided. When a compression spring is compressed, its diameter gets larger. Thus, the inside diameter of a hole enclosing the spring must be greater than the outside diameter of the spring to eliminate rubbing. An initial diametral clearance of one-tenth of the wire diameter is recommended for springs having a diameter of 0.50 in (12 mm) or greater.
  • 21. Materials Used for Springs Virtually any elastic material can be used for a spring. However, most mechanical applications use metallic wire—high-carbon steel (most common), alloy steel, .stainless steel, brass, bronze, beryllium copper, or nickel-base alloys. Most spring materials are made according to specifications of the ASTM.
  • 22. Types of Loading and Allowable Stresses The allowable stress to be used for a spring depends on the type of loading, the material, and size of the wire. Loading is usually classified into three types: Light service: Static loads or up to 10 000 cycles of loading with a low rate of loading (nonimpact). • Average service: Typical machine design situations; moderate rate of loading and up to 1 million cycles. Severe service: Rapid cycling for above 1 million cycles; possibility of shock or impact loading; engine valve .springs are a good example.
  • 23.
  • 24. Stresses and Deflections for Helical Compression Spring As a compression spring is compressed under an axial load, the wire is twisted. Therefore, the stress developed in the wire is torsional shear stress, and it can be derived from the classical equation 𝜏 = 𝑇𝑐/𝐽. When the equation is applied specifically to a helical compression spring, some modifying factors are needed to account for the curvature of the spring wire and for the directshear stress created as the coils resist the vertical load. Also, it is convenient to express the shear stress in terms of the design variables encountered in springs.
  • 25. Stresses and Deflections for Helical Compression Spring The resulting equation for stress is attributed to Wahl. The maximum shear stress, which occurs at the inner surface of the wire, is 𝜏 = 8𝐾𝐹𝐷𝑚 𝜋𝐷𝑚 3 = 8𝐾𝐹𝐶 𝜋𝐷𝑤 2 These are two forms of the same equation as C = Dm/Dw. Normally we will be concerned about the stress when the spring is compressed to solid length under the influence of Fs and when the spring is operating at its normal maximum load, Fo. Notice that the stress is inversely proportional to the cube of the wire diameter. This illustrates the great effect that variation in the wire size has on the performance of the spring.
  • 26. Stresses and Deflections for Helical Compression Spring The Wahl factor, K. in Equation is the term that accounts for the curvature of the wire and the direct shear stress. Analytically, K is related to C: 𝐾 = 4𝐶 − 1 4𝑐 − 4 + 0.615 𝐶 Figure shows a plot of K versus C for round wire. Recall that C = 5 is the recommended minimum value of C. The value of K rises rapidly for C < 5.
  • 27.
  • 28. Deflection Because the primary manner of loading on the wire of a helical compression spring is torsion, the deflection is computed from the angle of twist formula: 𝜃 = 𝑇𝐿 𝐺𝐽 Where 𝜃 = angle of twist in radians T = applied torque L = length of the wire G = modulus of elasticity of the material in shear J = polar moment of inertia of the wire
  • 29. Deflection Because the primary manner of loading on the wire of a helical compression spring is torsion, the deflection is computed from the angle of twist formula: 𝜃 = 𝑇𝐿 𝐺𝐽 Where 𝜃 = angle of twist in radians T = applied torque L = length of the wire G = modulus of elasticity of the material in shear J = polar moment of inertia of the wire
  • 30. Linear Deflection For convenience, we will u.se a different form of the equation in order to calculate the linear deflection, f of the spring from the typical design variables of the spring. The resulting equation is 𝑓 = 8𝐹𝐷𝑚 3 𝑁𝑎 𝐺𝐷𝑤 4 = 8𝐹𝐶3 𝑁𝑎 𝐺𝐷𝑤
  • 31.
  • 32. Buckling The tendency for a spring to buckle increases as the spring becomes tall and slender, much as for a column. Figure shows plots of the critical ratio of deflection to the free length versus the ratio of free length to the mean diameter for the spring. Three different end conditions are described in the figure. As an example of the use of this figure, consider a spring having squared and ground ends, a free length of 6.0 in, and a mean diameter of 0.75 in. We want to know what deflection would cause the spring to buckle.
  • 33. Buckling First compute 𝐿𝑓 𝐷𝑚 = 6.0 0.75 = 8.0 from Figure, the critical deflection ratio is 0.20.
  • 34. Buckling From this we can compute the critical deflection: That is, if the spring is deflected more than 1.20 in, the spring should buckle.
  • 35. Analysis of Spring Characteristics This section demonstrates the use of the concepts developed in previous sections to analyze the geometry and the performance characteristics of a given spring. Assume that you have found a spring but there are no performance data available for it. By making a few measurements and computations, you should be able to determine those characteristics. One piece of information you would have to know is the material from which the spring is made so that you could evaluate the acceptability of calculated stress levels.
  • 36. Example Problem 1 A spring is known to be made from music wire, ASTM A228 steel, but no other data are known. You are able to measure the following features using simple measurement tools: Free length = Lf = 1.75 in Outside diameter = OD = 0.561 in Wire diameter = Dw = 0.055 in The ends are squared and ground. The total number of coils is 10.0. This spring will be used in an application where the normal operating load is to be 14.0 lb. Approximately 300 000 cycles of loading are expected.
  • 37. Example Problem 1 For this spring, compute and/or do the following: 1. The music wire gage number, mean diameter, inside diameter, spring index, and Wahl factor. 2. The expected stress at the operating load of 14.0 lb. 3. The deflection of the spring under the 14.0-lb load. 4. The operating length, solid length, and spring rate. 5. The force on the spring when it is at its solid length and the corresponding stress at solid length. 6. The design stress for the material; then compare it with the actual operating stress. 7. The maximum permissible stress; then compare it with the stress at solid length. 8. Check the spring for buckling and coil clearance. 9. Specify a suitable diameter for a hole in which to install the spring.
  • 43. Design of Helical Compression Springs The objective of the design of helical compression springs is to specify the geometry for the spring to operate under specified limits of load and deflection, possibly with space limitations, also. We will specify the material and the type of service by considering the environ ment and the application.
  • 44. Example Problem 2 A helical compression spring is to exert a force of 8.0 lb when compressed to a length of 1.75 in. At a length of 1.25 in, the force must be 12.0 lb. The spring will be installed in a machine that cycles slowly, and approximately 200 000 cycles total are expected. The temperature will not exceed 200°F. The spring will be installed in a hole having a diameter of 0.75 in. For this application, specify a suitable material, wire diameter, mean diameter, OD, ID, free length, solid length, number of coils, and type of end condition. Check the stress at the maximum operating load and at the solid length condition.
  • 45. Example Problem 2 (Solution 1) The procedure works directly toward the overall geometry of the spring by specifying the mean diameter to meet the space limitations. The process requires that the designer have tables of data available for wire diameters and graphs of design stresses for the material from which the spring will be made. We must make an initial estimate for the design stress for the material by consulting the charts of design stress versus wire diameter to make a reasonable choice. In general, more than one trial must be made, but the results of early trials will help you decide the values to use for later trials.
  • 46. Example Problem 2 (Solution 1) Step 1: Specify a material and its shear modulus of elasticity, G. For this problem, several standard spring materials can be used. Let's select ASTM A231 chromium-vanadium steel wire, having a value of G = 11 200 000 psi. Step 2: From the problem statement, identify the operating force, Fo the operating length at which that force must be exerted, Lo ; the force at some other length, called the installed force, FI : and the installed length. LI. Remember, Fo is the maximum force that the spring experiences under normal operating conditions.
  • 47. Example Problem 2 (Solution 1) Many times, the second force level is not specified. In that ca.se, let FI = 0, and specify a design value for the free length, LF in place of LI. For this problem, FO= 12 lb; LO = 1.25in; FI = 8 lb; and LI = 1.75in. Step 3: Compute the spring rate, k 𝑘 = 𝐹𝑂 − 𝐹𝐼 𝐿𝐼 − 𝐿𝑂 = 12 − 8 1.75 − 1.25 = 8𝑙𝑏/𝑖𝑛 Step 4: Compute the free length, L, 𝐿𝐹 = 𝐿𝐼 + 𝐹𝐼 𝑘 = 1.75 + 8 8 = 2.75𝑖𝑛
  • 48. Example Problem 2 (Solution 1) The second term in the preceding equation is the amount of deflection from free length to the installed length in order to develop the installed force, FI. Of course, this step becomes unnecessary if the free length is specified in the original data. Step 5: Specify an initial estimate for the mean diameter, Dm Keep in mind that the mean diameter will be smaller than the OD and larger than the ID. Judgment is necessary to get started. For this problem, let's specify Dm = 0.60 in. This should permit the installation into the 0.75-in-diameter hole.
  • 49. Example Problem 2 (Solution 1) Step 6: Specify an initial design stress. The charts for the design stresses for the selected material can be consulted, considering also the service. In this problem, we should use average service. Then for the ASTM A231 steel, as shown in Figure, a nominal design stress would be 130 000 psi. This is strictly an estimate based on the strength of the material. The process includes a check on stress later Step 7: Compute the trial wire diameter. Notice that everything else in the equation is known except the Wahl factor K, because it depends on the wire diameter itself. But K varies only little over the normal range of spring indexes, C. From Figure, note that K = 1.2 is a nominal value. This, too, will be checked later.
  • 50. Example Problem 2 (Solution 1)
  • 51. Example Problem 2 (Solution 1) With the assumed value of K, some simplification can be done:
  • 52. Example Problem 2 (Solution 1) Step 8: Select a standard wire diameter from the tables, and then determine the design stress and the maximum allowable stress for the material at that diameter. The design stress will normally be for average service, unless high cycling rates or shock indicate thatsevere service is warranted. The light service curve should be used with care because it is very near to the yield strength. In fact, we will use the light service curve as an estimate of the maximum allowable stress. For this problem, the next larger standard wire size is 0.0625 in, no. 16 on the U.S. Steel Wire Gage chart. For this size, the curves in Figure for ASTM A231 steel wire show the design stress to be approximately 145 000 psi for average service, and the maximum allowable stress to be 170 000 psi from the light service curve.
  • 53. Example Problem 2 (Solution 1)
  • 54. Example Problem 2 (Solution 1)
  • 55. Example Problem 2 (Solution 1)
  • 56. Example Problem 2 (Solution 1)