[0001] This invention relates to a synchronous vibratory hammer employing a driving and
a driven eccentric weight arranged to produce vibratory action which may be used for
impacting a tool upon a work surface.
[0002] The art of vibratory hammers, of the type with which this invention is concerned,
is well developed and many different designs have been proposed and employed with
varying degrees of success. U.S. Patent No. 3,866,693, dated February 18, 1975 to
Bernard A. Century, is representative of one such vibratory hammer.
[0003] The subject invention has certain elements in common with the device of the Century
patent, however, it differs in at least one important respect, namely, it has no mechanical
restraints which can absorb energy, such as would be caused by the guides 186 and
188 of Century's patent. The mechanical restraints in the Century patent are used
to control non-linear motion of the hammer element being driven by a single eccentric.
The device of the subject invention eliminates the need for such mechanical restraints
because of the fact that two eccentrics are used.
[0004] The device of the subject invention requires less maintenance than vibratory hammers
having non-linear impacting vibrations, which not only shake the hammer supporting
mechanism, but are subject to greater wear and breakage.
[0005] A primary purpose of the invention is to provide a vibratory hammer with improved
operating efficiency, and which minimizes maintenance costs.
[0006] These and further purposes and features of the invention will become more apparent
from an understanding of the following disclosure with reference to the drawings as
set out in the respective figures thereof. From the drawings, it will be seen that
Fig. 1 is a side elevation view of a vibratory hammer embodying the principles of
the invention;
Fig. 2 is an enlarged section view as seen from line 2-2 in Fig. 1;
Figs. 3, 4 and 5 are cross section views as seen from lines 3-3, 4-4 and 5-5 respectively
in Fig. 2;
Fig. 6 is an exterior view of a hammer body component used in the device of Fig. l.
[0007] Referring now to Figs. 1 and 2, numeral 1 identifies a vibratory hammer having a
support frame consisting of a pair of side plates 3, which are maintained in parallel
position by means of tubular space bars 5, welded to the plates, as well as a tool
holder element 7, similarly welded thereto. A hammer body assemblage 9 (Fig. 6) is
suspended between the side plates 3 by resilient means consisting of four rubberrmounts
11 affixed to the side plates and the hammer body assemblage by means of bolts 13
and 15. As will be apparent, the mounts serve as the sole guiding and damping means
for the assemblage when the latter is vibrated during tool operation.
[0008] The hammer body assemblage 9 includes an eccentric weight chamber 17 enclosing a
pair of eccentric weights 19 and 21, mounted upon shafts 23 supported in roller bearings
25 positioned in end caps 27, the latter being secured by bolt means 29 to side members
31 of the eccentric weight chamber 15 by bolts 32. Projecting from the top surface
of the eccentric weight chamber 17 and affixed thereto, is an upper arm member 33
adapted to be affixed to the rubber mounts 11 by the bolts 15.
[0009] Projecting from the bottom surface of the eccentric weight chamber 7 and affixed
thereto, is a lower arm member 35 adapted to the rubber mounts 11 by the bolts 15.
Brace members 37 are secured to the sides of the lower arm member 35 and the hammer
body assemblage 9, to stabilize the arm member. An hydraulic motor 39, affixed to
the end of shaft 23, is provided to rotate the eccentric weight 19. A pair of gears
41, mounted upon the shaft 23, is arranged to transmit rotary motion from the shaft
which supports eccentric weight 19; to the shaft which supports eccentric weight 21,
so that both weights are rotated at the same speed, but in opposite directions. Hose
means 43 supply pressurized hydraulic fluid to the motor 39 when desired, from a power
source, not shown.
[0010] At the lower extremity of the arm member 35 is a striker plate 45 affixed thereto
by means of pin 47. The striker plate is arranged to impact upon a conical tool 49
mounted in the tool holder element 7 as best seen in Fig.
[0011] 2. Retaining means, including a key 51 projecting into a slot 53'formed in the tool
49, allow reciprocal movement of the tool. The tool slides in bushings 55 supported
in a bushing housing 57, the latter positionally maintained against axial movement
by a tool stop plate 59, affixed to the end of the tool holder by means of cap screws
61.
[0012] Support means for the vibratory hammer 1, are provided by a pivotally attached linkage
assemblage 63, which may be operatively positioned by power machinery, e.g., tractor,
not shown.
[0013] The design parameters of a vibratory hammer built in accordance with the invention
disclosed herein, obviously will vary in accordance with the work impact output desired.
[0014] It is to be recognized that when a forcing frequency vibrates a mass at its natural
frequency, the mass of the forcing frequency generator leads the vibrated mass by
90°. When the forcing frequency is much higher than the natural frequency, the forcing
frequency mass could lead the vibrated mass by 180°. Accordingly, if the leading phase
is 135
0, the vertical component of centrifugal force of the vibrated mass, coupled with the
stored energy of the rubber mounts, will produce maximum impacting on the tool 49.
[0015] The optimum phase angle of 135
0 (θ) is determined by the following equation:
where
θ = phase angle
§= damping factor
f = forcing frequency.CPM, RAD/SEC
fn = natural frequency
[0016] It can be demonstrated by plotting frequency ratio vs. θ with varying damping factors,
that anything less than a critically damped system gives phase angles of approximately
180° at any frequency ratio greater than 1, hence, critical damping of the system
is essential for optimum operative results. Critical damping by definition means no
over oscillation when a mass is deflected from its static position and returned to
the same static position. Critical damping is achieved by a preload, in the present
vibratory hammer, by use of the rubber mounts 11.
[0017] It is essential, for optimum operation, that the stroke of the hammer be equal to
the "in the air" displacement (S"), which is provided by the following equation:
Where w = unbalanced weight r = radius where unbalanced weight is located from the
center of rotation W = total weight vibrated
[0018] By application of these formula, a vibratory hammer in accordance with the invention
will have the following numeral values, if a work impact output of 200 ft. - lbs.
at 1200 rpm is to be achieved:
1. A vibratory impact hammer including a support frame characterized by a hammer body
assemblage suspended within the support frame by resilient means arranged to provide
guiding and damping action in either direction of axial movement of the hammer body
assemblage, said resilient means being the sole means engaging the hammer body assemblage
so that extraneous frictional forces are avoided, vibration drive means arranged to
vibrate the hammer body assemblage in an axial direction, and a tool reciprocably
mounted in the support frame and positioned to receive impact blows of the hammer
body assemblage when reciprocated by the vibratory drive means.
2. A vibratory impact hammer as in claim 1, characterized in that said resilient means
are rubber mounts.
3. A vibratory impact hammer as in claimsl or 2, characterized in that said rubber
mounts are arranged in pairs, one above the hammer body assemblage, the other below
the hammer body assemblage.
4. A vibratory impact hammer as in claim 1, characterized in that said vibratory drive
means includes a driving eccentric weight and a driven eccentric weight, and a motor
means arranged to rotate the weights in synchronism.
5. A vibratory impact hammer as'in any one of claims 1-4, characterized in that said
eccentric weights are inter-connected by gear means.
6. A vibratory impact hammer as in claim 1, characterized in that a tool holder is
provided for the tool, which tool holder includes means for removal of the tool from
the hammer.
7. A vibratory impact hammer as in claim 1, characterized in that the phase angle
of the forcing frequency leads the vibrated mass frequency by 135°.
8. A vibratory impact hammer as in any one of claims 1-7 characterized in that the
stroke of the hammer body assemblage is equal to 2 wr , wherein w = unbalanced weight,
r = radius where nhal ace is located from the center of rotation, and W = total weight
vibrated.
9. A vibratory impact hammer as in any one of claims 1-8, characterized in that a
hammer with a work impact output of 200 ft. - lbs. at 200 rpm, would have a stroke
of 0.4144 inches (1.052 cm) and design parameters as follows: