1. Rotating Unbalance
(Rotors, whose C.G. is not coinciding with the axis of shaft).
At time, t
fun in a particular direction,
fun = (MRotor eω2)
where, f0 = (mRotor eω2) — max volume of unbalanced force.
ω — force frequency or excitation.
2. Reciprocating Unbalance: (in Piston-crank)
fun = mRrω2 sinθ
[mR—mass of Reciprocating Ports]
(mass of Piston + mass of crosshead + mass of connecting Rod)
Where, ω = forced frequency and m = machine mass (whole) which is under vibrations.
3. Forced-Damped Systems (Perfect Reality)
Forced vibrations of a damped spring mass system
This is the equation of forced-Damped System.
∴ The solution will be, x = c · f + P · I
After some time, CF = 0
After solving,
Amplitude of forced vibrations (A):
Hence, x = PI
∴ x = A sin(ωt - ϕ)
Where, A = Amplitude of steady state vibrations (independence of time) (forced vibrations)
Running system vibrations will never stop.
Every machine/mechanical running system must have one running life.
4. Magnification factor (M.F.)
∴ M.F. depends upon:
(i) ω/ωn
(ii) ζ
Magnification Factor
Note: At some time 't',
F = f0sin[ωt]
x = Aω cos ωt
= Aω[sin{π/2 + (ωt - ϕ)}]
The Basic Equation was,
6. Vibration Isolations
It is used to isolate the ground from the vibrations of the Running machine so as to save other stationary m/cs from these vibration effects.
Vibration Isolation
Fτ = force transmitted to the ground
Fτ < < < < < F0
∈ = Fτ / F0 = Transmissivity
0 < ∈ < 1
∈ → 0 (for Belts)
Now, Fτ = Resultant of forces of spring force and damping force (max values)
Hence, ′∈′ depends upon:
(i) ω/ωn
(ii) ζ
Note: If, w/wn = 0 w/wn = √2 ⇒ ∈ = 1
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