Dynamic two frequency vibration damper

Claim 2

A dynamic vibration damper comprising: flexible bar; means for fixing the bar in a cantilever position onto a structural element with vibrations to be attenuated; and a pendulum connected rigidly to the bar, said pendulum being provided with means including a mass (m) for defining a first eigenfrequency of vibration (f 1 ), and for imparting to said pendulum a moment of inertia (J m ) around an axis perpendicular to an axis of said bar in a rest position of said bar, selected so as to define a second eigenfrequency of vibration (f 2 ) of the damper at a pre-fixed value which is an integral multiple of the first eigenfrequency (f 1 ).

Claim 3

The damper according to claim 1, wherein said second eigenfrequency (f 2 ) is equal to twice said first eigenfrequency (f 1 ).

Claim 4

The damper in accordance with claim 1, wherein said pendulum includes a cup element which lies on said axis of said bar and is connected to said bar by an end plate of the cup element which is set at an end of said cup element opposite to said structural element.

Claim 5

The damper according to claim 3, wherein said means for fixing includes a supporting element which can be connected to said structural element and is equipped with a seat for axial insertion of said bar, the bar being locked to the supporting element by a laser weld.

Claim 6

The damper according to claim 1, which includes tuning means for setting at least one of said eigenfrequencies (f 1 , f 2 ).

Claim 7

The damper according to claim 5 wherein said tuning means includes at least one ring nut which can be moved axially along an outer wall of said cup element.

Claim 8

The damper according to claim 6, further comprising a device for blocking said ring nut in a selected axial position.

Claim 9

The damper according to claim 7 wherein said device is at least one weld point.

Claim 10

The damper according to claim 6, which includes at least a pair of said ring nuts screwed onto an external thread formed on said cup element, the ring nuts being tightened together so as to lock them into position.

Claim 11

The damper according to claim 9 which includes two pairs of said ring nuts.

Claim 12

A vibration damper for a structural element of an aircraft having a fundamental frequency of vibration and a harmonic which is an integral multiple of the fundamental frequency, said damper comprising: a support element affixed to said structural element and provided with a hole; a circular cross section bar having one end received in said hole and fixed to said support element and cantilevered by said support element on said structural element, said bar being elastically deformable in flexure and in torsion; and a pendulum on an opposite end of said bar, said pendulum being in the shape of a cup open toward said support element and having a transverse wall receiving said opposite end of said bar and affixed thereto at an end of said cup turned away from said support element, said cup having a cylindrical externally threaded wall and being provided with a tuning ring threaded onto said wall and axially displaceable therealong, means being provided to fix said ring on said wall in a position in which the damper is tuned, said pendulum having means including a mass (m) for defining a first eigenfrequency of vibration (f 1 ) corresponding to said fundamental frequency and for imparting to said pendulum has a moment of inertia (J M ) around an axis perpendicular to an axis of said bar in a rest position of said bar selected so as to define a second eigenfrequency of vibration (f 2 ) corresponding to said harmonic.

Claim 13

A vibration damper for a structural element of an aircraft having a fundamental frequency of vibration and a harmonic which is an integral multiple of the fundamental frequency, said damper comprising: a support element affixed to said structural element and provided with a hole; a circular cross section bar having one end received in said hole and fixed to said support element and cantilevered by said support element on said structural element, said bar being elastically deformable in flexure and in torsion; and a pendulum on an opposite end of said bar, said pendulum being in the shape of a cup open toward said support element and having a transverse wall receiving said opposite end of said bar and affixed thereto at an end of said cup turned away from said support element, said cup having a cylindrical externally threaded wall and being provided with a tuning ring threaded onto said wall and axially displaceable therealong, means being provided to fix said ring on said wall in a position in which the damper is tuned, said pendulum having means including a mass (m) for defining a first eigenfrequency of vibration (f 1 ) corresponding to said fundamental frequency and for imparting to said pendulum has a moment of inertia (J M ) around an axis perpendicular to an axis of said bar in a rest position of said bar selected so as to define a second eigenfrequency of vibration (f 2 ) corresponding to said harmonic.

Claim 14

The vibration damper defined in claim 11 wherein said structural element has a hole extending through said structural element between opposite sides thereof, said support element being provided with a flange juxtaposed with one side of said structural element and a threaded shank extending through said hole in said structural element to an opposite side thereof, said damper further comprising: an internally and externally threaded bushing threaded onto said shank; a nut threaded onto said bushing and clamped against said structural element; another bar of circular cross section having one end received in and fixed to said bushing and cantilevered by said bushing on said structural element; another pendulum having a cup shaped configuration open in the direction of said bushing and formed with a transverse wall anchored to said other bar, each of said pendulums being provided with two pairs of internally threaded tuning rings thereon locked against one another for tuning the respective pendulums to said first and second eigenfrequencies respectively.