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Welcome to our Physics lesson on Combination of Springs, this is the third lesson of our suite of physics lessons covering the topic of Elastic Potential Energy and Combination of Springs, you can find links to the other lessons within this tutorial and access additional physics learning resources below this lesson.
The large value of spring constant obtained in the previous exercise, means the spring is very stiff and therefore, it can store a lot of elastic energy when stretched or compressed in maximum.
To change the level of stiffness in springs, we can combine two or more spring in two basic ways:
In this combination, the springs are placed one after another. As a result, when we hang an object on such a system, it pulls each spring if there was only one spring available. Therefore, the same weight causes a double extension in the system composed by two springs in series than if it was one spring only. Look at the figure below. For simplicity, the springs are taken as identical, i.e. they have a constant k each.
Since there is the same force F = m × g that acts in both cases, we have for the single spring system:
and for the double spring system:
This allows us to find a formula for the spring constant ks in series combination of springs. It is
where k1 and k2 are the constants of each spring respectively.
This rule can also extend for a system composed by more than two springs or when the springs are not identical, i.e. when their individual constants are different.
Two springs are combined in series as shown in the figure. The maximum extension of each spring without losing the elastic properties is 20 cm and 40 cm respectively.
Therefore,
and
Therefore, the system can hold 800 N at maximum so that both springs preserve their elastic properties.
Remark! Series combination of springs is usually applied when the springs available are stiffer than needed because combining two springs in series reduces the stiffness of the system, making it more elastic.
When two or more springs are connected in parallel, they distribute the load amongst them and as a result, they will extend less than if there was only one spring available. Such a combination creates a system of springs with a higher stiffness. The equation for the spring constant of the system of two parallel springs is
where kp is the spring constant of the parallel setup, while k1 and k2 are the constants of the individual springs.
In other words, if a single spring with constant k stretches by x units when an object m is hanged on it, then when we use two springs of this kind connected in parallel to hang the same object, they will extend by x/2 because the stiffness of the system increases by a factor of two. As a result, it can store double of energy it could store when a single spring was used. Look at the figure.
Two identical springs by constants 2000 N/m each, are combined in parallel.
For simplicity, take g = 10 N/kg.
We can take the figure shown above in theory as a reference. First, we must calculate the constant of the parallel system of springs. We have
a. The force caused in this system of spring is equal to the weight of the hanged object. Thus,
Therefore, the extension of the parallel system of springs is
b. The energy stored in this system of springs is calculated through the formula of elastic potential energy. We have:
Remark! The energy stored in this system of springs is different (is smaller) than if only one spring was used. Indeed, for the same force, if we had only one spring the extension would be
As a result, the energy stored in this spring would be
As you see, the energy stored is double of the one stored in the parallel setup, confirming the theory explained earlier.
In this case, we start by calculating the constant of the parallel part and then, we think as having a single spring in that part. It is combined in series with the rest of the springs to get the total spring constant of the entire system. Look at the figure:
For simplicity, we will consider only identical springs. If the mass of the springs and the support are not considered, there is only one force acting on the system. It is the object's weight. Therefore, the constants will be 2k for the parallel part and k for the lower spring, which is in series with the other two. As a result, the total spring constant of the system is
Therefore,
As for the total extension of the system, we have
You have reached the end of Physics lesson 5.4.3 Combination of Springs. There are 3 lessons in this physics tutorial covering Elastic Potential Energy and Combination of Springs, you can access all the lessons from this tutorial below.
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