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Elasticity is the ability of a material to recover its original shape and size after the force deforming it has been removed. For example, a rubber band snaps back to its original size after being stretched as shown in Fig. 7.1 (a). Similarly, a metre rule straightens up when a slight bending force is withdrawn.
Fig. 7.1: Elasticity of a rubber band and a metre rule A material is said to be more elastic if it gets back more precisely to its original shape and size. A piano wire, for example, is more elastic than a rubber band. Coil springs, also called helical springs (since their mathematical shape is called helix) are also elastic. When a spring is stretched by a force, it increases in length; more and more as the force increases. Generally, the applied force is proportional to the amount of extension, as described by Hooke’s Law. However, there is a limit to the size of the force beyond the material will permanently deformed. This limit is called elastic limit. Material that get permanently deformed when a force is applied on them are no-elastic. Examples of non-elastic materials include plasticine, dough and soap.
The requirements are; a spring with a pointer, six 50 g masses with hooks, retort stand with clamp and a metre rule. Suspend the spiral spring on the stand with the pointer at the bottom Clamp the metre rule retort stand close to the spring Note and record in a table the initial pointer reading ( x 0 ) on the metre rule. See Fig. 7.2 (a). Hook one 50 g mass on the spring, just below the pointer, note and record the new pointer reading ( x 1 ). See Fig. 7.2 (b). Determine the extension ( e ) of the spring from the two values. e = x 1 - x (^0) Repeat this with the addition of one 50 g mass at a time Plot a graph of force against extension of the spring
Fig. 7.2: Investigating the relationship between force and extension
Table 7-1: Table of data Original position of the spring when no mass is attached = x 0 Mass (g) Force (N) Pointer position (cm)
Extension (e) ( x 1 - x 0 ) cm 50 0.5 x 1 100 1.0 x (^2) 150 1.5 x (^3) 200 2.0 x (^4) 250 2.5 x 5 300 3.0 x (^6)
Fig. 7.3: Force against extension graph sketch A straight line through the origin has a constant gradient and it implies that the components plotted are directly proportional. It can therefore be concluded that the extension of a spring is directly proportional to the force attached. This relationship is described by Hooke’s law.
It describes the relationship between extension of a stretching material and the stretching force. It states that The extension of a spring is directly proportional to the applied force, provided that the elastic limit of the spring is not exceeded
This law can be mathematically expressed as;
In the equation, k is the constant of proportionality and is called the springs constant. A spring with a large spring constant is stiffer and extends just a little when a force is applied to it. Graphically, Hooke’s law can be represented as shown in Fig. 7.4 below.
Fig. 7. Form the graph;
Example 7. A body of mass 560 g causes an extension of 2.8 mm to a certain copper wire. Determine the mass that will cause a 3.6 mm extension on the same wire given that the wire obeys Hooke’s law. Solution
5.6 (^) 2.0 /
3.6 2 7.
F ke k F^ N N mm e mm When e mm F N
Example 7. A spring obeying Hooke’s law was suspended on a fixed support. When a load of 6 N load was hung on it, the length of the spring was 18 cm. When a 30 N load was hung on it, the length increased to 30 cm. Determine: a. the length of the spring without a load b. the length of the spring when supporting a load of 20 N. Solution a. In this case, a force of 24 N (30 N – 6 N) produces an extension of 12 m (30 cm -18 cm) Determine the extension produced by the 5 N (^6 ) 2 e F cm k
Original length pf the spring = 18 cm – 3 cm =15 cm b. Determine the extension for 20 N (^20 ) 2
e F cm k
Add to the original length Length=10 + 15 cm = 25 cm
Spring constant can be likened to the stiffness of a spring. A spring that is stiffer has a large spring constant. Consider two cases below:
1. A force of 5 N extends spring P by 25 cm. We determine the spring constant by applying
1
F ke k F^ N e m Nm
With a large value of k, spring Q requires more force to extend by the same value as P. Spring Q is thus stiffer than P.
2. A force of 20 N extends spring Q by 25 cm.
1
F ke k F^ N e m Nm
The stiffness (spring constant increases) increases with the decrease in diameter. Spring C is stiffer than spring D.
A spring made of a thicker wire is stiffer than the one made of thin wire of the same material. F has stiffer than E
Test yourself 7.
Force (N) 0 2 4 6 8 10 12 14 16 Extension (cm) 0.0 1.6 3.2 5.0 6.4 7.8 9.6 11.2 12.
a. Use these results to plot a graph of force against extension b. Determine the spring constant of the spring from the graph c. Use the graph to find i. the force that produces and extension of 7.o cm ii. the extension when the force is 5 N
Work is done in stretching or compressing a spring. This work done is equivalent to the energy stored in the spring. The SI unit of work and energy is the Joule (J). The energy is called elastic potential energy and is given by;
2
Work done Energy stored Fe W E Fe ke
In the graph of force against extension, work done is equivalent to the area under the curve.
Fig. 7.5: Work done in stretching a spring
Example 7. A force of 50 N is used to stretch a certain spring through 8 cm. Calculate the elastic potential energy stored in the spring. Solution
Fig. 7. In this combination, the system is stiffer than a single spring. The spring constant is thus the sum of individual spring constants.
If the springs are identical, then the total extension is half the extension of a single spring.
(^2 ) t e e^ F k
Example 7. Determine total extension in the setup shown in Fig. 7.8. The springs are identical and the constant of proportionality (k) of each is 100 Nm -^.
Fig. 7.
Solution
1 2 1
k eq k k Nm e F m k
Alternatively;
t 2 2 100 e e m
Fig. 7.9 shows two springs connected in series. When a constant force, F is applied on spring 2, the springs are extended and the total extension is the sum of extension of each spring.
Fig. 7.9: Springs in series
1 2
1 2
1 2
Total extension e e e F F k k F k k
Therefore, for springs in series, effective spring constant k (^) eq, is given by,
Form Two Physics: By Mr. Njeka-0723054060. For: Girls at Coulson: “We all are smart in Physics” 8
1 2 3
k eq k k k
For two springs in series,
1 2 1 2 eq
k k k k k
Example 7. It is observed that a 160 g mass produces an extension 4 cm when attached on a spring. Determine the total extension produced when three such springs are connected in series and parallel, as shown in the figure below.
Fig. 7.
Solution Find the spring constant k
1
Using extensions; Extension of the top spring, e 1
1
e F m k
2 1 2
t
e e m e e e m
Using spring constants Spring constant for the two springs in parallel 1 k 1 (^) 2 k 80 Nm
The equivalent spring pf the system in series
1 2 1 1 2
eq 80 40 3
k k k Nm k k
t eq
Example 7. Given that the spiral springs in Fig. 7.11 below are identical with a spring constant of 200 N/m each, determine the total extension produced by the 300 N load.
Form Two Physics: By Mr. Njeka-0723054060. For: Girls at Coulson: “We all are smart in Physics” 10
Fig. 7. (a) What is the spring constant of the spring? (b) What force would cause two such springs placed in parallel to stretch by 10cm (c) State three factors that affect the proportionality constant of a helical spring.
Fig. 7. Determine the constant of each spring if the extension produced on the system is 10 cm.
Form Two Physics: By Mr. Njeka-0723054060. For: Girls at Coulson: “We all are smart in Physics” 11
Fig. 7.
Calculate; (a) The extension in one spring (b) The extensive proportionality constant of the springs