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// Use the foreach loop using System; class ForeachDemo { static void Main() { int sum = 0; int[] nums = new int[10]; // Give nums some values for(int i = 0; i < 10; i++) nums[i] = i; // Use foreach to display and sum the values foreach(int x in nums) { ConsoleWriteLine("Value is: " + x); sum += x; } ConsoleWriteLine("Summation: " + sum); } }

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The output from the program is shown here:

13:

Value Value Value Value Value Value Value Value is: is: is: is: is: is: is: is: 0 1 2 3 4 5 6 7

Plotting the displacement of the follower in Fig 128, we can nd the velocity and acceleration curves by employing the method of nite differences We nd a strong imposed frequency of acceleration of 41/2 cycles/sec It may be seen that the frequency ratio = 450 cycles sec = 18 1 rev sec 4

Part I:

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Value is: 8 Value is: 9 Summation: 45

Thus, by observation of Fig 128, we see that the chatter is caused by (a) resonance between natural frequency and the strong eighteenth harmonic number and (b) excessive jerk values, especially at the dwell ends of the cam curve A new cam designed with a smoother acceleration curve with smaller maximum jerk values solved the problem by yielding weaker higher harmonics

As this output shows, foreach cycles through an array in sequence from the lowest index to the highest Although the foreach loop iterates until all elements in an array have been examined, it is possible to terminate a foreach loop early by using a break statement For example, this program sums only the first five elements of nums:

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// Use break with a foreach using System; class ForeachDemo { static void Main() { int sum = 0; int[] nums = new int[10]; // Give nums some values for(int i = 0; i < 10; i++) nums[i] = i; // Use foreach to display and sum the values foreach(int x in nums) { ConsoleWriteLine("Value is: " + x); sum += x; if(x == 4) break; // stop the loop when 4 is obtained } ConsoleWriteLine("Summation of first 5 elements: " + sum); } }

1234 Two-Degree-of-Freedom System Let us consider a two-degree-of-freedom linear, closed-track cam-follower system as shown in Fig 129 For other applications of two DOF systems, see Hanachi and Freudenstein (1986) and Eliss (1964) Let m1, m2 = respective mass: 1, 2, lb k1, k2 = respective spring, 1, 2, lb/in b1,b2 = respective damping coef cient, 1, 2, lb/(in/sec)

This is the output produced: