# Connexions

You are here: Home » Content » Work by spring force

### Recently Viewed

This feature requires Javascript to be enabled.

# Work by spring force

Module by: Sunil Kumar Singh. E-mail the author

Summary: Nature of spring force is to restore its configuration.

Note: You are viewing an old version of this document. The latest version is available here.

Spring is an arrangement, which is capable to apply force on a body. As we will see, spring force is similar to gravity in many important ways. At the same time, it is different to gravity in one important way that it applies a variable force unlike gravity.

Though work by spring is expected to vary as we stretch or compress a spring, but just like gravity, the work by spring force for a given displacement is constant and is independent of the presence of other force(s). We shall analyze work by a spring in various situations, but with a difference. In this case, we shall first outline the characterizing aspects of spring and then develop an expression for work. Subsequently, we shall analyze situations first with spring force alone and then along with other external force(s) on similar line as in the case of work by gravity.

Since the nature of spring force is very much alike gravity, the treatment in the module may appear similar to that for the work by gravity.

## Spring force

Spring force is given by the expression :

F = - k x F = - k x

where k is spring constant, measured experimentally for a particular spring. The value of k (=-F/x) measures the stiffness of the spring. A high value indicates that we would require to apply greater force to change length of the spring.

This relationship, defining spring force, is also known as “Hooke’s law”, which is valid under two specific conditions :

1. The mass of spring is negligible (and can be neglected).
2. There is no dissipative force (like friction) involved with spring.

The attribute “x” is measured from the position of “neutral length” or “relaxed length” - the length of spring corresponding to situation when spring is neither stretched nor compressed. We shall term this position as origin.

The negative sign in the expression indicates an important aspect of the nature of spring force that it is always directed towards the position at neutral length. See the figure to visualize how spring force is always directed towards origin.

### Cotext of spring force

We must, here, understand that forces on the body (block) attached to spring may involve friction, if the surfaces between block and the surface is rough. For the sake of simplicity, we consider here that the surfaces are smooth. In this situation, we need not consider force due to gravity as it is normal to the motion and does not influence our consideration. As such, we will not consider gravity, while calculating work for the motion on smooth surface.

Just like the case of gravity, there are two situations with respect to application of force on a body by the spring.

1: In one case, the body is given a jerk, say towards right and the body is let go. In this case, the only force on the block is spring force. This situation is similar to vertical projection of an object with an initial speed. This case of spring force, therefore, is specified by an initial speed, preferably at the origin.

2: In other case, there is external force(s) in addition to spring force. The horizontal component of the force is applied on the block as it moves along the surface. This situation is similar to the case of pulling a lift vertically by string and pulley arrangement. In this case, we would be required to analyze external force with the help of “free body diagram”.

## Work by spring force

Now, we are set to obtain an expression for the work done by the spring on a block as shown in the figure. We give the block a jerk to the right as discussed earlier. Let the extension of the spring be “x”. Then,

F = - k x F = - k x

As the force is variable, we can not use the expression “Frcosθ” to determine work. It is valid for constant force only. We need to apply expression, involving integration to determine work :

W S = F ( x ) x W S = F ( x ) x

Let x i x i and x f x f be the initial and final positions of the block with respect to origin, then

W S = x i x f - k x x W S = - k [ x 2 2 ] ] x i x f W S = 1 2 k ( x i 2 - x f 2 ) W S = x i x f - k x x W S = - k [ x 2 2 ] ] x i x f W S = 1 2 k ( x i 2 - x f 2 )

If block is at origin, then x i = 0 x i = 0 and x f = x x f = x (say), then

W S = - 1 2 k x 2 W S = - 1 2 k x 2

When block is subjected to the single force due to spring, the work is given by above two expressions. During motion towards right, the spring force on the block acts opposite to the direction of motion. It increases in magnitude with increasing displacement. Thus, spring force does negative work transferring energy "from" the block. As a consequence, kinetic energy of the block decreases.

This process continues till the velocity and kinetic energy of the block are zero. Spring force, then, pulls block towards the mean position i.e. in negative x - direction. The spring force, now, is in the direction of motion. It does the positive work on the block transferring energy to the block.

The process continues till the particle returns to the initial position, when its velocity is same as that in the beginning. As such kinetic energy of the block on return at mean position is equal to that in the beginning.

K f = K i K f = K i

For the roundtrip, net work by spring force is zero. Net transfer of energy “to” or “from” the particle is zero. Initial kinetic energy of the particle is retained at the end of round trip. Thus, we can see that the motion under spring is lot similar as that of motion under gravity.

### Example 1

Problem : A block of 1 kg is attached to the spring and is placed horizontally with one end fixed. If spring constant is 500 N/m, find the work done by the horizontal force to pull the spring through an extension of 10 cm.

Solution : This is a situation, when initial and final speeds are zero. This means that initial and final kinetic energies are zero (equal). Hence, work done by the two forces is zero. In this condition, work done by the horizontal force is equal to the work done by the spring force, but opposite in sign. Now work done by the spring force is :

W S = - 1 2 x 500 x 0.1 2 W S = - 2.5 J W S = - 1 2 x 500 x 0.1 2 W S = - 2.5 J

Thus, work done by the horizontal force is :

W S = 2.5 J W S = 2.5 J

## Motion with spring and other force(s)

We must understand that work by spring force, for a given displacement, is independent of the presence of other forces. The work done by spring remains same.

For this situation, “work-kinetic energy” theorem has following form :

K f - K i = W S + W F K f - K i = W S + W F

where W S W S and W F W F are the work done by the spring force and other applied force(s) respectively.

Here, work done by other external force(s) may be analyzed with respect to following different conditions :

1. Initial and final speeds are zero.
2. Initial and final speeds are same.
3. Initial and final speeds are different.

In the first two cases, initial and final kinetic energy are same. Hence,

K f - K i = W S + W F = 0 W F = - W S K f - K i = W S + W F = 0 W F = - W S

This is an important result. This means that we can simply compute the work done by spring force and assign the same preceded by a negative sign as the work done by other force(s). Such situation can arise when external force displaces the block and extends the spring to a certain extension such that end velocities are either zero or same.

In third case, kinetic energies at end points are not same. However, work done by spring force remains same as before. Thus, the difference in kinetic energy during a motion is attributed to the net work as done by spring and other forces.

### Example 2

Problem : A block of 1 kg with a speed 1 m/s hits a spring placed horizontally as shown in the figure. If spring constant is 1000 N/m, find the compression in the spring.

Solution : When block hits the spring, it is compressed till the block stops. Here, we see that kinetic energies at the beginning and at the point when block stops are not same. Note that the only force acting on the block is due to spring. Hence,

K f - K i = W S K f - K i = W S

W S = K f - K i = 0 - 1 2 m v 2 W S = - 0.5 x 1 x 1 2 = - 0.5 J W S = K f - K i = 0 - 1 2 m v 2 W S = - 0.5 x 1 x 1 2 = - 0.5 J

Now, work by spring is :

W S = - 1 2 k x 2 W S = - 0.5 x 1000 x x 2 = - 500 x x 2 W S = - 1 2 k x 2 W S = - 0.5 x 1000 x x 2 = - 500 x x 2

Combining two values, we have :

- 250 x x 2 = - 0.5 - 250 x x 2 = - 0.5

x 2 = 0.5 500 = 0.001 x = 0.032 m x 2 = 0.5 500 = 0.001 x = 0.032 m

## Content actions

### Give feedback:

My Favorites (?)

'My Favorites' is a special kind of lens which you can use to bookmark modules and collections. 'My Favorites' can only be seen by you, and collections saved in 'My Favorites' can remember the last module you were on. You need an account to use 'My Favorites'.

| A lens I own (?)

#### Definition of a lens

##### Lenses

A lens is a custom view of the content in the repository. You can think of it as a fancy kind of list that will let you see content through the eyes of organizations and people you trust.

##### What is in a lens?

Lens makers point to materials (modules and collections), creating a guide that includes their own comments and descriptive tags about the content.

##### Who can create a lens?

Any individual member, a community, or a respected organization.

##### What are tags?

Tags are descriptors added by lens makers to help label content, attaching a vocabulary that is meaningful in the context of the lens.

| External bookmarks