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Chapter 8 Vibration. A. Free vibration = 0. k. Undamped free vibration. m. x. n = ( k / m ) 1/2 : natural frequency C : amplitude o : initial p hase angle x o : initial displacement, x o = C sin( o ) T : period, such that T n =2, or T = 2 / n
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Chapter 8 Vibration A. Free vibration = 0 k Undamped free vibration m x n= (k/m)1/2: natural frequency C : amplitude o : initial phase angle xo : initial displacement, xo= C sin(o ) T : period, such that Tn =2, or T = 2 /n f : frequency = 1/T
Damped free vibration : k m • Define viscous damping constant c (N s/m) x Use a trial solution x = A et:
overdamped z > 1, Critical damped z = 1 underdamping z < 1 x decays to zero without oscillation • Case 1: Overdamped when > 1, such that +and-< 0
Case 2: Critical damping when = 1 += - = -n • General solution : x = (A1+ A2t )exp(-nt) • x approaches zero quickly without oscillation.
Case 3: Underdamped< 1 Period d = 2/d
Experimental guideline: • Measure and n • Calculate • Calculate viscous damping constant c according to • = c/(2mn)
B. Forced vibration of particles : The equation of motion :
Maximum M occurs at: The resonance frequency is
tan = Consider the following regions: (1) is small, tan > 0, 0+, xp in phase with the driving force (2) is large, tan < 0, 0-, = , xp lags the driving force by 90o (3) n-, tan +, /2(-) n+, tan -, /2(+)
If the driving force is not applied to the mass, but is applied to the base of the system: If b2 is replaced by Fo/m: This can be used as a device to detect earthquake.
Example m =45 kg,k = 35 kN/m, c = 1250 N.s/m, p = 4000 sin (30 t) Pa, A= 50 x 10-3 m2. Determine : (a) steady-state displacement (b) max. force transmitted to the base.
The force transmitted to the base is : For max Ftr :