Horizontal block-spring system

The Hooke’s law governing an ideal spring relates spring force with displacement as :

F = - k x F = - k x

Figure 1: The spring is stretched a bit and then let go to oscillate.

Horizontal block-spring system

Combining with Newton’s second law,

⇒ F = m a = - k x ⇒ F = m a = - k x

⇒ a = - k m x ⇒ a = - k m x

Now, comparing with SHM relation “ a = - ω 2 x a = - ω 2 x ”, we have :

⇒ ω = k m ⇒ T = 2 π m k ⇒ ν = 1 2 π k m ⇒ ω = k m ⇒ T = 2 π m k ⇒ ν = 1 2 π k m

In these expressions “m” and “k” represent inertia and spring factor respectively.

Vertical block-spring system

Vertical block-spring system differs to horizontal arrangement in the application of gravitational force. In horizontal orientation, gravitational force is perpendicular to motion and as such it is not considered for the analysis. In vertical orientation, however, the spring is in extended position due to the weight of the block before the block is set in SHM. It is in equilibrium in the extended position under the action of gravitational and spring force.

Clearly, the center of oscillation is the position of equilibrium. The block oscillates about the extended position – not about the position of neutral spring length as in the case of horizontal arrangement. Let us consider that the spring is extended by a vertical length “ y 0 y 0 ” from neutral position when it is in equilibrium position. For a further extension “y” in spring, the spring force on the block is equal to the product of spring constant and total displacement from the neutral position,

F = - k y 0 + y F = - k y 0 + y

Figure 2: The spring is stretched a bit from the equilibrium position and then let go to oscillate.

Vertical block-spring system

Note that we have considered downward displacement as positive. The spring force acting upward is opposite to displacement and hence negative. In this case, however, the net restoring force on the block is equal to the resultant of spring force acting upwards and gravity acting downward. Considering downward direction as positive,

⇒ F net = F + m g = - k y 0 + y + m g ⇒ F net = F + m g = - k y 0 + y + m g

But, for equilibrium position, we have the following relation,

m g = - k y 0 m g = - k y 0

Substituting this relation in the expression of net restoring force, we have :

⇒ F net = - k y ⇒ F net = - k y

The important point to realize here is that net restoring force is independent of gravity. It is equal to differential spring force for the additional extension – not the spring force for the total extension from the neutral position. Now, according to Newton’s second law of motion, the net restoring force is equal to the product of mass of the block and acceleration,

⇒ F net = m a = - k y ⇒ F net = m a = - k y

⇒ a = - k m y ⇒ a = - k m y

This relation on comparison with SHM equation “ a = - ω 2 x a = - ω 2 x ” yields same set of periodic expressions as in the case of horizontal block-spring arrangement :

⇒ ω = k m ⇒ T = 2 π m k ⇒ ν = 1 2 π k m ⇒ ω = k m ⇒ T = 2 π m k ⇒ ν = 1 2 π k m

In this case, however, we can obtain alternative expressions as well for the periodic attributes as spring force at equilibrium position is equal to the weight of the block,

m g = - k y 0 m g = - k y 0

Dropping negative sign and rearranging,

⇒ m k = y 0 g ⇒ m k = y 0 g

Hence, the alternative expressions of periodic attributes are :

⇒ ω = g y 0 ⇒ T = 2 π y 0 g ⇒ ν = 1 2 π g y 0 ⇒ ω = g y 0 ⇒ T = 2 π y 0 g ⇒ ν = 1 2 π g y 0

Clearly, the extension of the spring owing to the weight of the block in vertical orientation has no impact on the periodic attributes of the SHM. One important difference, however, is that the center of oscillation does not correspond to the position of neutral spring configuration; rather it is shifted down by a vertical length given by :

⇒ y 0 = m g k ⇒ y 0 = m g k

Block connected to springs in series

We consider two springs of different spring constants. An external force like gravity produces elongation in both springs simultaneously. Since spring is mass-less, spring force is same everywhere in two springs. This force, however, produces different elongations in two springs as stiffness of springs are different. Let “ y 1 y 1 ” and “ y 2 y 2 ” be the elongations in two springs. As discussed for the single spring, the net restoring force for each of the springs is given as :

F net = - k 1 y 1 = - k 2 y 2 F net = - k 1 y 1 = - k 2 y 2

Figure 3: The spring is stretched a bit from the equilibrium position and then let go to oscillate.

Block connected to springs in series

The total displacement of the block from equilibrium position is :

⇒ y = y 1 + y 2 = - F net k 1 − F net k 2 ⇒ y = y 1 + y 2 = - F net k 1 − F net k 2

⇒ F net = k 1 k 2 y k 1 + k 2 ⇒ F net = k 1 k 2 y k 1 + k 2

A comparison with the expression of extension of the single spring at equilibrium position reveals that spring constant of the arrangement of two springs is equivalent to a single spring whose spring constant is given by :

⇒ k = k 1 k 2 k 1 + k 2 ⇒ k = k 1 k 2 k 1 + k 2

This relationship can also be expressed as :

⇒ 1 k = 1 k 1 + 1 k 2 ⇒ 1 k = 1 k 1 + 1 k 2

In the nutshell, we can consider the arrangement of two springs in series as a single spring of spring constant “k”, which is related to individual spring constants by above relation. Further, we can extend this concept to a number of springs by simply extending the relation as :

⇒ 1 k = 1 k 1 + 1 k 2 + 1 k 3 + … ⇒ 1 k = 1 k 1 + 1 k 2 + 1 k 3 + …

The periodic attributes are given by the same expressions, which are valid for oscillation of single spring. We only need to use equivalent spring constant in the expression.

Block in between two springs

In this arrangement, block is tied in between two springs as shown in the figure. In order to analyze oscillation, we consider oscillation from the reference position of equilibrium. Let the block is displaced slightly in downward direction (reasoning is similar if block is displaced upward). The upper spring is stretched, whereas the lower spring is compressed. The spring forces due to either of the springs act in the upward direction. The net downward displacement is related to net restoring force as :

F net = - k 1 y 1 - k 2 y 2 = − k 1 + k 2 y F net = - k 1 y 1 - k 2 y 2 = − k 1 + k 2 y

Figure 4: The spring is stretched a bit from the equilibrium position and then let go to oscillate.

Block in between two springs

A comparison with the expression of extension of the single spring reveals that spring constant of the arrangement of two springs is equivalent to a single spring whose spring constant is given by :

⇒ k = k 1 + k 2 ⇒ k = k 1 + k 2

Clearly, the periodic attributes are given by the same expressions, which are valid for oscillation of single spring. We only need to use equivalent spring constant in the expression.

Block connected to springs in parallel

Here, we consider a block is suspended horizontally with the help of two parallel springs of different spring constants as shown in the figure. When the block is pulled slightly, it oscillates about the equilibrium position. The net restoring force on the block is :

F net = - k 1 y 1 - k 2 y 2 = − k 1 + k 2 y F net = - k 1 y 1 - k 2 y 2 = − k 1 + k 2 y

Figure 5: The spring is stretched a bit from the equilibrium position and then let go to oscillate.

Block connected to springs in parallel

A comparison with the expression of extension of the single spring reveals that spring constant of the arrangement of two springs is equivalent to a single spring whose spring constant is given by :

⇒ k = k 1 + k 2 ⇒ k = k 1 + k 2

Again, the periodic attributes are given by the same expressions, which are valid for oscillation of single spring. We only need to use equivalent spring constant in the expression.