Can we achieve linearity in helical springs like in cantilever design?

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Helical springs can exhibit linear behavior similar to cantilevers, particularly when designed with cylindrical, uniform coils that have not begun to close. The spring force across a contact surface is generally linear, influenced by factors such as end treatment and coil pitch. While helical springs are predominantly made from a single wire for ease of manufacturing, there is potential for designs using multiple wires, although this adds complexity and cost. Helical springs can function in both tension and compression, but typically serve one purpose based on design needs. The discussion also touches on the calculation of natural frequencies for helical springs, suggesting a need for specific equations to define their behavior.
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For the design of a cantilever, assuming a Hookean material is used below its proportionality limit, stress will be proportional to strain. From this we can conclude that its behavior will be linear.

However, how can we apply this knowledge towards helical springs? Is it possible to design a helical spring whose linearity approaches or equals the cantilever?

Thanks,
Thadman
 
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Yes, typical, cylindrical, uniform, helical springs, whose coils have not started to close, have approximately linear behavior, like the cantilever.
 
nvn said:
Yes, typical, cylindrical, uniform, helical springs, whose coils have not closed, have approximately linear behavior, like the cantilever.

Assuming a cylindrical, uniform, helical spring, whose coils have not started to close, which supports a surface. Would the spring force be linear across the contact surface?
 
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I don't know the shape of the contact force curve on the contact surface. I think the shape of the contact force curve would probably tend to vary depending on the spring end treatment (wire shape and pitch).
 
yes springs are linear and full contact as the top and bottom is " flat " or they can be made without the " flat" ends

see link below for more infohttp://www.hypercoils.com/
 
After some brief research, I see that a variety of helical spring topologies are utilized in designs. However, I'm still unable to find an example of a multiple arm, helical compression spring. All of the examples I'm aware of involve a single arm. Is there a reason for this?

Can the compression spring operate equally in compression as well as expansion?
 
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Hi thadman,
thadman said:
After some brief research, I see that a variety of helical spring topologies are utilized in designs. However, I'm still unable to find an example of a multiple arm, helical compression spring. All of the examples I'm aware of involve a single arm. Is there a reason for this?

Can the compression spring operate equally in compression as well as expansion?
What do you mean by a "multiple arm" spring? Are you referring to a type of disk spring?
http://www.mcmaster.com/#disc-springs/=3pweox

There are a lot of different types of springs, but the most common use a single wire wound into a helix. The spring constant remains constant over the usable range of the spring unless it's specifically made not to. In other words, helically wound springs produce a force that is very linear with respect to displacement. They are commonly used in both tension and compression.
 
Q_Goest said:
There are a lot of different types of springs, but the most common use a single wire wound into a helix. The spring constant remains constant over the usable range of the spring unless it's specifically made not to. In other words, helically wound springs produce a force that is very linear with respect to displacement. They are commonly used in both tension and compression.

I was wondering why a single wire is often used as compared to multiple wires.

Is the single wire simply easier to manufacture? Does it offer benefits compared to multiple wires?

Helical springs are often used in either compression or tension, why not both? If the spring was rigidly coupled to 2 parallel plates, couldn't it function both in tension as well as compression?

As far as visualizing a multiple arm helical spiral, imagine a multiple arm logarithmic spiral and the differences that exist between it and a logarithmic spiral.

(multiple arm) http://1.bp.blogspot.com/_SqhhJb_P3...I/TJksEbXxyo4/s400/blue,+green+spiral+top.gif

(single arm)
http://www.cs.princeton.edu/introcs/32class/images/logspiral.png

A multiple arm, helical spring would simply use multiple wires would into a helix
 
I've seen helical springs that are nested, one inside another (ie: one diameter is larger than the other) but I've not seen them made with two wires of the same diameter as you've suggested. I could be done, just take 2 identical springs and orient them 180 degrees apart. They couldn't be closed and ground for obvious reasons, but it would work if you had end plates made up to accommodate the end configuration.

Looks like there's an advantage to doing this actually. Comparing 2 springs with 1, both with the same total spring rate, the 2 springs will have less stress for any given load than the single spring.

The problem is it adds a lot of complexity and cost to a design.

Springs can be made to handle both tension and compression but that's generally not needed. If there were some design reason to produce a spring that works in both compression and tension, it wouldn't be a big deal to design it like that.
 
  • #10
I picked up the seventh edition of Roark's formulas for Stress and Strain. It appears to be rather trivial to calculate the fundamental resonance for a helical spring. However, calculating the mass normalized modes does not appear to be trivial.

Assuming a cantilever (left end fixed, right end free), an equation exists which defines all of the natural frequencies.

F(x)=(K(n)/2pi)*sqrt(EIg/wl^4)

Where K(n) = 3.52 for the 1st mode (n=1), 22 for the second mode (n=2), 61.7 for the third mode (n=3), 121 for the fourth mode (n=4), 200 for the fifth mode (n=5), etc.

Nodal position wrt length = .783 for the 2nd mode (n=2), .504/.868 for the third mode (n=3), .358/.644/.905 for the fourth mode (n=4), .279/.5/.723/.926 for the fifth mode (n=5), etc

How can we define a similar equation for a helical spring?
 
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  • #11
With regards to my previous posts,

For defining the natural frequencies of a beam rigidly coupled at both ends, we are given the equation:

F(X)=(Kn/2pi)*sqrt(EI/Rho*A*(L^4))

where:
Kn=mode number
E=elastic modulus
I=area moment of inertia (ie second moment of inertia, I believe)
Rho=mass density
A=cross sectional area
L=length

However, what second moment of inertia equation do we want? I believe we can calculate it with respect to both X and Y, where (assuming a rectangular cross-section) I(x)=b(h^3)/12 and I(y)=h(b^3)/12 and h=height (ie y) and b=width (ie x).
 
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