HVT1 Simple Pendulum
A simple pendulum consisting of a cord
with a ring at the top end and a sliding pendulum
mass.
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HVT3 Compound Pendulum
A wall mounted bracket has a metre long bar
suspended from its knife-edge pivot point. Attached
to the pendulum bar is a movable mass. The mass can
be fixed along the pendulum bar in seven positions.
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HVT2 Reversible Pendulum
The reversible pendulum
consists of a rigid metal bar with two pivot points,
one near each end of the bar. It can be suspended
from either pivot and swung. The two pivots are
adjustable on the rigid metal bar and this allows
the periods of swing to be adjustable. In use, it is
swung from one pivot, and the period timed, and then
turned upside down and swung from the other pivot,
and the period timed.
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HVT9 Torsional Vibration
Apparatus
The equipment provides a basic range of torsional
vibration experiments. A wire rod clamped in a wall
mounted bracket has a heavy disc attached to the
lower end. A solid ring can be located over the disc
to increase its inertia. Steel and brass rods of two
different diameters are included. All brackets,
clamps and adapters are supplied.
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HVT11 Vibration of a Spiral
Spring
Spiral springs are used to provide a restoring
torque to an oscillating shaft when it rotates
through an angular displacement. With this apparatus
the student can easily calculate the theoretical
simple harmonic motion of the spring, and compare
the value with experimental results. The wall
mounted unit consists of a spiral spring coiled from
a length of steel strip creating an effective
length, attached to a shaft mounted in ball
bearings. A cord carrying a load hanger is wound
around the shaft, and a load applied to twist the
spring. Spring deflection is measured with an
attached 360° scale. A cord and load hanger is
supplied. A set of inertia discs is supplied which
can be attached to the shaft to change the frequency
of oscillation, measured by the stop watch provided.
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HVT12c Beam Bending (Transverse)
Vibration Module
Experimental module for the vibration analysis of
transverse beam bending. The apparatus consists of
two end fixings that support a beam. One end allows
beam rotation only, whilst the other end allows
rotation and horizontal movement only. The beam is
forced to vibrate using a clamp on motor exciter
supplied. This exciter operates from a high speed
motor and has two eccentric masses attached at
either end of the motor shaft. The rotation of the
masses induces the excitation frequency of the beam.
Additional masses can be added to the motor exciter
to change the experimental parameters. The vibration
of the beam is monitored using the sensor of the
HAC190.
The HAC190 optional accessory is required to
control the speed of the motor exciter and the
HVT12k optional accessory to display the excitation
frequency and output frequency.
Optional Accessories: HAC190,
HVT12k, HVT12f
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HVT12d Vibration Absorber
Experimental module, which fits into the HVT12f
Vibrations frame (not supplied) making up part of
the HVT12 Universal Vibration Apparatus.
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HVT12e Vibration Sensors with
Fixing Kit, Interface & Softwa
Sensor and clamping kit for use on some of the
linear and torsional vibrations apparatus within the
Hitech range.
Two sensors supplied; Linear non-contact position
sensor and contacting angular position sensor.
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HVT12f Vibrations Frame
The HVT12f Vibration Frame offers the ideal
working frame for all of the HVT12 Universal
Vibration experiment modules. Manufactured from high
quality, ergonomic aluminium profile, it comprises
solid side profiles for rigidly mounting experiment
components. Dual upper and lower members create
internal working dimensions of 1.22m x 0.76m for
mounting experiments. Profile grooves create an
accurate alignment of experiment components, and
pre-assembled fasteners are integrated into the
grooves for assembling of specific experiments
within the HVT12 range. The HVT12f Vibrations Frame
comes fully assembled with no need for tooling or
lengthy assembly.
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HVT12g Free and Forced Vibrations
A rectangular steel cantilever beam pivots at one
end from a bracket and bearing. A spring is attached
to the free end of the beam. The horizontal position
of the beam can be adjusted. Beam displacement is
measured using the sensor of the HAC190. The beam
vibrates freely by displacing the free end by a
known amount between the two bump stops provided.
Alternatively the beam can be forced to vibrate
using the HAC120 Motor Exciter. The motor exciter
has integral imbalanced masses, which when rotated
excites the beam to vibrate. The frequency of the
beam excitation is controlled and displayed using
the HAC190 speed controller and tachometer. A set of
calibrated weights are supplied to vary the weight
being vibrated. Damping is introduced onto the beam
using a set of damping discs and damping tank. Input
and output excitations can be viewed using the
optionally available HVT12k Data Acquisition
Interfaceand software
Optional Accessories: HAC120, HAC190, HVT12k,
HVT12f
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HVT12h Mass Spring System
A single open helical spring is mounted inside
the HVT12f Vibrations Frame and free to vibrate
vertically through a linear bearing guide. Loading
is achieved through the use of various masses.
Masses are added to the lower end of the spring to
vary the frequency of oscillation. Frequency,
periodic time and deflection can be measured. An
upper adjustment system allows the springs vertical
position to be varied and thus its deflection
increased and decreased.
Full technical instruction manual included
detailing apparatus assembly, operation, and theory
and example results.
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HVT12k Data Acquisition System
This unique and compact Data Acquisition System
is an essential accessory for the HVT12 Universal
Vibrations Apparatus experiments. When connected to
the relevant experiment and its sensors, the system
allows measuring, capturing, storing and analysing
of experiment data.
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HVT13 Torsional Vibration
Apparatus
This bench top mounted unit is used to study
torsion and torsional vibration. The apparatus is
constructed around a profiled aluminium base onto
which are mounted 4 vertical chuck pillars. Each
pillar contains a central shaft running in precision
bearings with a chuck at one end which grips a
torsion specimen. Each chuck also contains a large
disc of varying mass and inertia. With these chucks
it is possible to assemble a torsion specimen with
up to 3 masses. Vibrations are transmitted into the
torsion specimen by means of an exciter, which is
electronically speed controlled from the main
control unit. Angular movement sensors on the chuck
pillars provide the amplitude of vibration as an
electrical signal. The control unit conditions these
signals and makes them available to view on the
HVT13k Data Acquisition System. Static twist of the
specimen is achievable using the attachable
protractor, pointer, hanger and calibrated weights
supplied.
Optional Accessories: HVT13k
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HVT14 Spring Mass Vibration
System
The floor standing unit is used to analyse the
oscillations of a spring mass system. The sturdy
base secures two vertical guides. A top horizontal
bracket keeps the bars at a near constant width
which aids the running of a cradle up and down the
bars. The cradle runs on integral precision bearings
which creates minimal friction. The cradle attaches
to one end of a helical tension spring of known wire
diameter, free length and spring rate. At the other
end of the spring an adjustable screw mechanism
adjusts the length of the spring and hence it’s
starting position. The cradle has its own self
weight, but additionally a number of calibrated
weights can be added to the cradle in order to vary
the oscillating mass. The cradle vertical motion is
transferred to a rotating drum recorder mounted with
paper. The paper can be removed after testing to
undertake further analysis. The oscillations of the
cradle can be free or damped. The damped option
requires the damper to be attached to the cradle.
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HVT20 Stability of Structures
Apparatus
This apparatus enables a number of simple models,
each with a single degree of freedom to be
assembled. Each of the models constructed will
exhibit a specific type of behavior which because of
the extensibility of the springs is not limited to
the linear load/deflection range common in most
laboratory equipment.
Students also have sufficient flexibility to
devise and construct their own models. In this way
an understanding of the non-linear stability
behavior of thin structures may be achieved along
with the analysis of the buckling of practical
structures. A model strut consisting of two rigid
links connected by a pinned joint is mounted in a
test frame with a fixed pin at one end and a pin
free to move axially at the other.
The rigidity of the strut is achieved by
attaching various linear coil springs or a torsion
spring to the centre pin or the free end. The free
end is constrained by a loading yoke that is guided
by linear bearings running on parallel rails. The
central joint is fitted with a trunnion to which
loading cables are connected. One cable includes a
strain gauged load cell to measure the net force
being applied. The signal from the strain gauge load
cell is fed into the Data Acquisition Interface
supplied. The set of weights needed for the
experiment is provided.
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HAC90 Tachometer
A bench top unit that operates in conjunction
with the HVT12 Universal Vibration System. This unit
display the excitation frequency (in Hz) of the
motor exciter being used to excite the beam. This
module will operate with both the HAC120 (sold
separately) and motor exciter from the HVT12c
(supplied with HVT12c). The digital display shows
the excitation frequency in units of Hz and to a
resolution of 1 decimal place.
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HAC110 Speed Controller
The HAC110 makes up an essential control
component of the HVT12 Universal Vibrations
Apparatus. It connects directly to the HAC90 –
Tachometer (sold separately) and also the HAC120 –
Motor exciter (sold separately) and motor exciter of
the HVT12c (sold as part of HVT12c experiment
module).
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HAC120 Motor Exciter
The HAC120 exciter motor is an essential part of
the HVT12 Universal Vibration Apparatus (sold
separately).
Its primary function is to transmit rotational
motion into linear displacement of a beam, and hence
force the beam to vibrate at varying amplitudes and
frequencies.
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