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Note that Y*(l) = Y(1,1,l) The dynamic error Z is de ned as the difference between the actual and the static follower responses Let k = wn/w, where wn is the natural frequency of a one degree-offreedom elastic model of the cam-follower system and w is the rotational speed of the cam Neglecting damping, the governing equation of Z is assumed to be Z + k 2 Z = a( d , b ,q ) (1362)

ConsoleWriteLine(); // Use a Nybble in an int expression t = a * 2 + 3; ConsoleWriteLine("Result of a * 2 + 3: " + t); ConsoleWriteLine(); // Illustrate int assignment and overflow a = 19; ConsoleWriteLine("Result of a = 19: " + (int) a); ConsoleWriteLine(); // Use a Nybble to control a loop ConsoleWriteLine("Control a for loop with a Nybble"); for(a = 0; a < 10; a++) ConsoleWrite((int) a + " "); ConsoleWriteLine(); } }

The output from the program is shown here:

The absence of a damping term in Eq 1362, required for the method developed here, is usually conservative The amplitude of the residual vibration induced by the rise curve is then R( k ) = 1 A( d , b , k ) k (1363a)

30 20 10 _6 _4 _2 _ 10 _ 20 _ 30 2 4 6 _6 _4 _2

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a: 1 b: 10 a is less than b c after c = a + b: 11 a after a += 5: 6 Result of a * 2 + 3: 15 Result of a = 19: 3 Control a for loop with a Nybble 0 1 2 3 4 5 6 7 8 9

Although most of the operation of Nybble should be easy to understand, there is one important point to make: The conversion operators play a large role in the integration of Nybble into the C# type system Because conversions are defined from Nybble to int and from int to Nybble, a Nybble object can be freely mixed in arithmetic expressions For example, consider this expression from the program:

Because v is de ned to be zero for q < 0 and q > b, Eq (1363a) becomes R( k ) = V ( d , b , k ) (1363b)

t = a * 2 + 3;

Here, t is an int, as are 2 and 3, but a is a Nybble These two types are compatible in the expression because of the implicit conversion of Nybble to int In this case, since the rest of the expression is of type int, a is converted to int by its conversion method

30 20 10 2 _ 10 _ 20 _ 30 4 6

The residual response spectrum is thus the Fourier spectrum of the velocity curve v(d,b,q) The area of an admissible velocity curve between q = 0 and b is equal to the follower rise d Convolution, h(q), of two functions f(q) and g(q) is de ned as h(q ) = f * g = In the transform plane, H (l ) = F(l ) G(l ) (1364b)

Part I:

13:

+ -

One other point: Syntactically, when a finally block follows a try block, no catch clauses are technically required Thus, you can have a try followed by a finally with no catch clauses In this case, the finally block is executed when the try exits, but no exceptions are handled

Fig 136(b)

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