Phil Hobbs <
pcdhSpamM...@electrooptical.net> wrote:
> On 07/21/2017 05:15 PM, rickman wrote:
>> Phil Hobbs wrote on 7/21/2017 3:00 PM:
>>> Hi, all,
>>>
>>> I'm designing a mixed-signal board for a fire safety system intended
>>> to go on large pieces of agricultural equipment. It's doing DSP-type
>>> things, so it needs a decent clock.
>>>
>>> Naturally I thought of using an external XO. However, these gizmos
>>> are liable to have a pretty rough life, with lots of vibration and
>>> impact and stuff.
>>>
>>> Sooo, what do you use for a +-50 ppm, low jitter oscillator that will
>>> survive being dropped on the ground from a few metres up?
> > Why do you think this will be a problem.
> Because I've broken crystals by dropping them on the floor in the past.
> Not SMT ones, which is why I asked.
> Cheers
> Phil Hobbs
SMT may be your answer. Some excerpts:
SMT military oscillator withstands 100,000-g shock
IQD's HGXO Series of surface mount oscillators is designed primarily
for military applications such as smart munitions and projectile
electronics although the devices can also be used in demanding
industrial applications. Designed around a hermetically sealed
high-shock crystal and a CMOS compatible integrated circuit, the new
device is able to survive shock levels of up to 100,000 g and
vibration levels of 20g at 10-2000 Hz swept sine in accordance with
MIL-STD-202G. Housed in an industry standard 7-mm x 5-mm four-pad
ceramic package with metal lid, five supply voltage versions are
available at 5.0 V, 3.3 V, 3.0 V, 2.5 V and 1.8 V, thus providing
compatibility with the latest generation of low power chipsets.
Output frequencies can be specified between 460 kHz and 5 MHz with a
15-pF HCMOS drive capability. Frequency tolerance is available down
to +/-10 ppm whilst frequency stability can be specified at +/-40
ppm over the full military temperature range of -55 C to 125C down
to +/-10 ppm over commercial temperature ranges coupled with low
frequency ageing characteristics.
https://www.ecnmag.com/product-release/2013/07/smt-military-oscillator-
withstands-100000-g-shock
High-shock quartz crystal oscillators
The classical quartz crystal oscillator is historically one of the
most fragile components in an electronic system. This is not
surprising since the quartz crystal resonator within the oscillator
was composed of a large crystal such as a large round-blank AT-cut
crystal mounted by metal clips inside of a metal housing. This
construction could not survive shocks much beyond 50 to 100 g. While
these crystal oscillators are superb for large benchtop instruments
and similar devices, they are not well suited for applications where
the device can expect high shocks such as handheld devices and
munitions. In these cases, the accelerations can be on the order of
thousands or even tens of thousands of g's. Clearly, the classical
construction is not adequate for these applications.
The impetus to change the construction of quartz crystals and
oscillators came from the continuing drive to miniaturize
electronics. A key step in this miniaturization took place in 1970
with the development of the photolithographic and chemical milling
processes for manufacturing quartz crystals. These processes,
adopted from those used in the silicon industry, allow the precise
milling of quartz crystals with dimensions under 1 mm and features
as precise as a few microns. Another important step in this
miniaturization was the development of the ceramic package for
firmly mounting the crystal in a rugged housing. Together, this
manufacturing and construction technique has become the de facto
standard for miniature quartz crystals.
Miniaturization vs. benefits
Fortunately, the miniaturization of the quartz crystal has had the
added benefit of greatly improving their shock and vibration
survivability. Because of its small size, the resonator has low
mass, and so the force on the resonator is low. Using strong
mounting materials, the resonator is held firmly in place - the
force due to acceleration is not sufficient to cause the crystal to
dismount. Further, because of its small size (short blank size or
short tuning-fork tines), the shear forces within the resonator are
low and hence they can survive high shocks without breaking.
Another added benefit of the small size is that the frequency of the
lowest flexure mode of the resonator can be on the order a few
kilohertz or higher. This has at least two benefits.
First, for shocks that have a characteristic time of about 1 ms or
longer, the shock can be treated as a quasi-static impulse - at any
given time the shock can be approximated as a static acceleration.
Because of this, the build-up in acceleration is sufficiently slow
that it does not excite the flexure modes of the crystal.
Second, since these flexure modes are high in frequency, they will
not be excited under vibration (which normally does not extend
beyond 2 kHz in typical applications). This is important in both
high-vibration applications and when manufacturing boards that are
cut out using a router.
http://www.electronicproducts.com/Passive_Components/Oscillators_Crystals_S
aw_Filters/High-shock_quartz_crystal_oscillators.aspx