IQD Frequency Products is a recognised market leader in Quartz Crystals, Clock Oscillators, Fast Make Oscillators, TCXOs, VCTCXOs, VCXOs, OCXOs, Rubidium Oscillators
2. History
2
Pre 1970 – High shock was a few 100g
1970s – resonators could survive shock
levels of a few 1,000g
1980s – 10,000g (HG products)
2000s – 100,000g CX4HG and HGXO
3. Two basic failure mechanisms
3
Dismount
Is the epoxy mount strong enough to hold
the resonator in place?
Breakage
Is the resonator design robust enough to
survive the stresses induced by high shock
events?
4. Keys to ruggedness
4
Small size
Smaller devices typically experience lower
stresses under acceleration
Stress length2/thickness
Maintain scale, then stress size
Fixed frequency, stress (length)2
Smaller size
Lower stress
Can withstand higher accelerations (shocks)
Mechanical support
Single end mount is good
Dual end mount is better
Lower stress
thickness
length
stress
2
Stress dual–end mounting = stress single–end mounting
6
1
5. Avoiding dismount
5
Shorten resonator
Shear dismount: Fixed frequency and
bonding area, 𝐴, (mass)∝(length),
so 𝐹 /𝐴∝ (length), so shorter resonator
is less likely to dismount
Peel dismount: Torque τ ∝ (length) x
(mass) ∝ ( length)2, so shorter resonator
is less likely to dismount
The right adhesive
Strong
Low outgassing
Doesn’t de-Q the resonator
Plenty of it
Dual-end mount, for AT (introduces
other issues)
Force distributed
6. Avoiding breakage
6
Simple geometry (avoiding weak structures)
Fairly easy for ATs
More challenging for tuning-forks
Small resonator (Stress length2/
thickness)
Dual-end mount (reduces stress)
7. Where we are today
7
AT crystals
Most products offer 10,000g or more
Some offer up to 100,000g
Could achieve 200,000g or more
Would pursue if there were a market
demand for this
Tuning-fork crystals
Many offer up to 5,000g
Up to 30,000g in preferred directions in some
cases
More information can be found on our
website www.iqdfrequencyproducts.com