Summary

Mechanism analysis or kinematics of machines is inherently a vital part in machine design.   The Slider Crank Chain is one of the two basics mechanisms that form the basis for many more complicated motions.  The other is the Four Bar Chain or Chebyshev linkage of which over 800 forms are known.  Using this Slider Crank Chain mechanism, the velocities can be find using the method of Instantaneous Centers.  The method is shown in the Theory section.

The purpose of this experiment is to obtain a graph of piston velocity against crank angle using the method of instantaneous centers, assuming that the crank rotates at a constant angular velocity and to obtain the crank angles which correspond to the maximum piston velocity.  Then, to show that for a slider crank chain the piston motion tends to approach simple harmonic motion with increasing values of connecting rod/crank ratio.  The apparatus used is the Slider Crank Chain with a variable connecting rod length mechanism apparatus, shown in the Appendix section.  With reference to the theory of the experiment, the result is obtained by rotate the crank by 10° increments and note the corresponding piston displacement and the cross-scale readings for five different connecting rod lengths: 115, 130, 140, 155 and 175 mm.  This step is repeated for a full 360° rotation.  The result of the experiment is tabulated and shown at the Data, Observation and Result section.  The graph of piston displacement and velocity against the crank angle for the five connecting rod is plotted in one graph in FIGURE 1 and FIGURE 2.  Below are the findings of the experiment:

·        The relationship between the piston velocity against the crank angle has a sinusoidal characteristic. 

·        The piston displacement against crank angle shows a quadratic characteristic. 

·        But, the two common characteristic from both figures are both the piston displacement and velocity will go back to its initial condition after completing one revolution cycle. 

·        For different connecting rod lengths, the ratio between connecting rod and crank radius is different.  Consequently, the point of maximum displacement will also different. 

·        The higher the ratio, the lower the maximum point of its displacement.

·        Maximum piston velocity for all the graph that were plotted occur at an angle of 80° and 280° instead of 90° and 270° as stated as the theoretical value.

·        The piston was under simple harmonic motion due to the fact that it was under the oscillating motion.  It has a maximum acceleration due to the increasing and decreasing of the piston velocity of the mechanism itself.

·        It is found that the maximum acceleration is about 0.3 mm/s2 and it occurred at an angle about 250° to 260°. 

·        The maximum acceleration and the maximum velocity do not occur at the same crank angle.  At the angle where the maximum velocity occurs, the acceleration must have a value of zero.

In conclusion, by using the method of instantaneous centers, the piston velocity is obtained and it is proved that the piston motion tends to approach simple harmonic motion with the increasing values of the corresponding rod/crank ratio. The experiment results showed that it tends to agree to the theoretical part of experiment.

 

Purpose / Objective

The purpose of this experiment is to obtain a graph of piston velocity against crank angle using the method of instantaneous centers, assuming that the crank rotates at a constant angular velocity and to obtain the crank angles which correspond to the maximum piston velocity.  Then, finally to show that for a slider crank chain the piston motion tends to approach simple harmonic motion with increasing values of connecting rod/crank ratio.

 

Procedures

1.      On the circular scale, set the crank to zero.

2.        Both knurled nuts are slacken and adjust the position of the piston pivot so that the connecting rod is 115 mm long.  Make sure that the spacer washer is between the piston and the connecting rod.  In normal use, the knurled nuts will be just slack.  However, the motion of the slider crank chain can be locked at any position by tightening both knurled nuts.

3.        Record the piston displacement and the cross-scale readings in table for every 10° of crank rotation.  Note that with the crank angle set to zero, note the initial reading of the cross-scale.  This will need subtracting from all subsequent readings in order to obtain the true reading.

4.        Steps 1 to 3 are repeated for connecting rod lengths of 130, 140, 155 and 175 mm.

Data, Observation and Result

 

The data for the piston displacement and piston velocity for the five different connecting rod lengths were shown in tables below.

 

Ø      Table 1:

Connecting rod length :

115 mm

 

 

Crank radius:

35 mm

 

 

Ratio :

3.3

 

 

 

 

 

 

Crank angle

Piston Displacement

Piston Velocity

 

(degrees)

(mm)

(mm/s)

 

0

60.0

0.0

 

10

60.5

-7.0

 

20

62.0

-14.0

 

30

65.5

-19.5

 

40

70.0

-24.0

 

50

75.0

-28.0

 

60

80.5

-30.0

 

70

86.0

-31.0

 

80

92.5

-31.0

 

90

98.5

-30.0

 

100

104.5

-28.0

 

110

111.0

-24.0

 

120

116.0

-21.0

 

130

120.0

-18.0

 

140

123.0

-14.0

 

150

122.0

-11.0

 

160

123.0

-7.0

 

170

129.5

-4.0

 

180

130.0

-1.0

 

190

130.0

3.0

 

200

128.0

7.0

 

210

127.0

11.0

 

220

124.0

14.0

 

230

121.0

17.0

 

240

117.0

21.0

 

250

112.5

24.0

 

260

107.5

26.5

 

270

100.0

30.0

 

280

93.5

31.5

 

290

87.0

32.0

 

300

80.0

30.0

 

310

74.5

28.0

 

320

70.0

24.0

 

330

62.5

19.5

 

340

62.5

14.0

 

350

60.5

7.0

 

360

60.0

0.0

 

 

Ø      Table 2:

Connecting rod length :

130 mm

 

Crank radius:

35 mm

 

Ratio :

3.7

 

 

 

 

Crank angle

Piston Displacement

Piston Velocity

(degrees)

(mm)

(mm/s)

0

44.5

0.0

10

45.0

-6.5

20

47.0

-13.0

30

50.0

-18.5

40

54.0

-23.0

50

59.0

-27.0

60

64.0

-29.0

70

70.0

-31.0

80

72.0

-31.0

90

83.0

-30.0

100

89.0

-28.0

110

96.0

-25.0

120

101.0

-22.0

130

105.0

-18.5

140

109.0

-15.0

150

111.0

-11.0

160

113.0

-8.0

170

114.5

-4.0

180

115.0

-1.0

190

115.0

4.0

200

114.0

7.0

210

112.0

11.0

220

109.0

15.0

230

105.5

19.0

240

102.0

22.0

250

97.0

25.0

260

91.0

28.0

270

84.5

30.0

280

78.0

32.0

290

71.0

31.0

300

65.0

30.0

310

60.0

27.0

320

55.0

24.0

330

51.5

20.0

340

48.0

13.5

350

45.5

7.0

360

44.5

0.0

 

 

 

 

 

 

 

 

 

Ø      Table 3:

 

Connecting rod length :

140 mm

 

Crank radius:

35 mm

 

Ratio :

4.0

 

 

 

 

Crank angle

Piston Displacement

Piston Velocity

(degrees)

(mm)

(mm/s)

0

35.0

0.0

10

35.5

3.5

20

37.5

-19.0

30

40.5

-23.5

40

44.5

-27.5

50

49.5

-29.5

60

55.0

-31.5

70

60.5

-31.5

80

67.0

-30.5

90

73.0

-26.5

100

78.5

-26.0

110

86.0

-23.0

120

90.0

-19.5

130

94.5

-16.0

140

98.0

-12.5

150

100.5

-8.5

160

103.0

-5.0

170

104.5

-1.0

180

105.0

3.5

190

105.0

7.0

200

104.0

10.0

210

102.0

11.0

220

99.0

15.0

230

96.0

19.0

240

91.5

22.0

250

87.0

25.5

260

81.5

28.0

270

74.5

30.5

280

68.5

32.0

290

61.5

32.0

300

56.5

30.0

310

49.5

27.5

320

45.0

23.0

330

41.0

18.5

340

38.0

13.0

350

36.0

6.0

360

35.0

0.0

 

 

 

 

 

 

 

Ø      Table 4:

 

Connecting rod length :

155 mm

 

Crank radius:

35 mm

 

Ratio :

4.4

 

 

 

 

Crank angle

Piston Displacement

Piston Velocity

(degrees)

(mm)

(mm/s)

0

20.0

0.0

10

20.0

-7.0

20

22.0

-13.5

30

25.0

-19.0

40

29.0

-23.5

50

34.0

-27.5

60

39.5

-30.0

70

45.0

-31.5

80

51.0

-32.5

90

57.0

-31.5

100

64.0

-29.5

110

70.0

-26.5

120

74.5

-24.0

130

79.5

-20.5

140

83.0

-17.0

150

86.0

-12.5

160

88.0

-9.0

170

89.0

-5.0

180

90.0

-1.0

190

90.0

4.0

200

89.0

8.0

210

87.0

12.0

220

84.0

16.0

230

80.0

19.5

240

76.0

23.0

250

71.0

26.0

260

64.5

29.0

270

59.0

31.0

280

53.0

32.0

290

46.0

32.0

300

39.5

30.0

310

34.5

28.0

320

29.5

23.5

330

25.5

19.0

340

22.5

13.5

350

20.5

6.0

360

20.0

0.0

 

 

 

 

 

 

 

Ø      Table 5:

 

Connecting rod length :

175 mm

 

Crank radius:

35 mm

 

Ratio :

5.0

 

 

 

 

Crank angle

Piston Displacement

Piston Velocity

(degrees)

(mm)

(mm/s)

0

0.5

0.0

10

0.5

-7.0

20

2.0

-13.5

30

5.3

-18.5

40

9.0

-23.5

50

14.0

-27.5

60

19.5

-30.5

70

25.0

-31.5

80

32.0

-32.0

90

37.0

-31.5

100

43.0

-30.5

110

49.5

-28.0

120

55.0

-24.5

130

59.5

-21.0

140

63.0

-17.5

150

65.5

-13.5

160

68.0

-9.5

170

69.5

-5.5

180

70.0

-1.5

190

70.0

3.5

200

69.0

8.5

210

67.0

13.0

220

64.0

17.0

230

60.0

21.0

240

56.0

24.5

250

51.0

27.0

260

45.5

29.5

270

38.5

31.5

280

32.5

32.0

290

26.0

32.0

300

20.0

30.0

310

14.5

27.0

320

9.5

23.5

330

5.5

18.0

340

2.5

12.5

350

1.0

6.0

360

0.5

0.0

 

 

 

From the data recorded, the graph of piston displacement and piston velocity against crank angle for the five different connecting rod lengths was plotted in one graph shown in FIGURE 1 and FIGURE 2, attached next page.

Discussion

            From the experimental data tabulated and the plotted graphs in FIGURE 1 and FIGURE2, the relationship between the piston displacement and velocity against the crank angle is obtained.  From FIGURE 2, it is clearly that the graph has a sinusoidal characteristic.  On the other hand, FIGURE 1 shows a quadratic characteristic.  But, the two common characteristic from both figures are both the piston displacement and velocity will go back to its initial condition after completing one revolution.  For different connecting rod lengths, the ratio between connecting rod and crank radius is different.  Consequently, the point of maximum displacement will also different.  The higher the ratio, the lower the maximum point of its displacement.  The experiment results showed that it tends to agree to the theoretical part of experiment.  With reference to FIGURE 2, it can be clearly seen that the graph has a sinusoidal characteristic.  But, there was not much different for five connecting rods in terms of their maximum and minimum velocity.  The slight difference or error occurred might be due to the inefficiency of the apparatus itself. 

Maximum piston velocity for all the graph that were plotted occur at an angle of 80° and 280° instead of 90° and 270° as stated as the theoretical value.  This showed that the error occurred in experiment has contributes the 10° difference.  Although there exist difference, it can be said that the experiment results tend to agree quite well with the theory. 

The piston was under simple harmonic motion due to the fact that it was under the oscillating motion.  It has a maximum acceleration due to the increasing and decreasing of the piston velocity of the mechanism itself.  The higher the value of the ratio would give a better shape and form of simple harmonic motion of the plotted graph.  The maximum acceleration occurs at the steepest slope among the plotted graph in FIGURE 2.  Based on it, it is quite hard to find by just looking at the graphs.  So, finding the best steepest slope of the plotted graphs will make an assumption.  It is found that the maximum acceleration is about 0.3 mm/s2 and it occurred at an angle about 250° to 260°.  The maximum acceleration and the maximum velocity do not occur at the same crank angle.  The simple relationship is obtained.  At the angle where the maximum velocity occurs, the acceleration must have a value of zero.

 

 

Conclusion

 

In conclusion, by doing the experiment of the slider crank chain, the characteristics of the mechanism is learned.  It can be said that these mechanisms form the basis for more complicated motions such as in the internal combustion engine mechanism.  By using the method of instantaneous centers, the graph of piston velocity against the crank angle is successfully plotted by assuming that the crank rotates at a constant angular velocity.  By analyzing the graph, the maximum piston velocity and maximum acceleration can be obtain easily.  Finally, it is proved that the piston motion tends to approach simple harmonic motion with the increasing values of the corresponding rod/crank ratio.