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Laboratory & cleanroom3 min readLast updated September 2026

Cryo-electron microscopy: why cooling must be constant, not powerful

A cryo-electron microscope needs little cooling, but that cooling must be extremely uniform. Anyone who assesses the task on the basis of the cooling load is planning past the actual requirement – and risks unusable measurement series.

Key points

  • The cooling load of a cryo-electron microscope is small; what matters is the stability of the cooling water temperature over time.
  • Even a temperature change of a tenth of a degree expands components by many times what the instrument is intended to resolve.
  • Stability specifications are often formulated as drift over a time window – they can be met economically with inertia, for example a buffer volume.
  • What is decisive is always the installation requirements of the specific instrument, not average values for the type of instrument.

01Little cooling, high requirement

Cryo-electron microscopes make individual proteins visible. For this, the sample is flash-frozen and kept below −170 °C with liquid nitrogen; from tens of thousands of individual images, a three-dimensional model is created with a resolution of a few ångströms, i.e. fractions of a nanometre. A measurement series often runs unattended for hours to days – an interruption can render the entire series worthless.

02The fallacy: cooling capacity instead of constancy

For building services engineering, the task initially looks small: per instrument, only a few kilowatts have to be removed to the cooling water, less than for some server cabinets. The magnetic lenses of the microscope, however, are current-carrying coils whose optical properties depend on their temperature. The cooling water therefore does not just keep the instrument cool, it keeps the optics stable.

03The principle: thermal expansion versus resolution

Metal expands with temperature. A simplified estimate shows the order of magnitude: half a metre of steel becomes around 0.6 micrometres longer when heated by 0.1 K – about three thousand times the target resolution.

Simplified estimate: a temperature change of 0.1 kelvin expands 0.5 metres of steel by 0.6 micrometres, approx. 3000 times more than the target resolution of 0.2 nanometresTHERMAL EXPANSION · SIMPLIFIED ESTIMATEΔL = α · L · ΔTα ≈ 12 · 10⁻⁶ 1/Ksteel, reference valueL = 0.5 massumed effective lengthΔT = 0.1 Ktemperature change0.1 nm1 nm10 nm100 nm1 µmlogarithmic scaletarget resolution · ≈ 0.2 nm (2 Å)expansion at 0.1 K · ≈ 0.6 µm× 3'000Even a tenth of a degree shifts components by many timeswhat the microscope is meant to resolve.
A tenth of a degree versus two ångströms Simplified estimate with typical value for steel and assumed length

Manufacturers therefore specify tight limits for the stability of cooling water and room temperature, often as a permissible change within a time window. For the room air, published facility descriptions state, for example, less than 0.8 K fluctuation over 24 hours.

04Inertia is cheaper than control quality

Whether a tolerance is formulated as an instantaneous band or as drift over a time window makes a big difference. Slow drift can be managed with inertia: a well-mixed buffer volume in the instrument circuit acts like a low-pass filter that smooths out rapid fluctuations from the chilled water network. A plate heat exchanger alone hardly achieves this; it separates systems, but does not dampen.

Fictitious calculation example: a network fluctuation of plus/minus 0.5 kelvin with a 10-minute period is damped by a buffer with a 20-minute time constant to approx. plus/minus 0.04 kelvinBUFFER VOLUME AS A LOW-PASS FILTER · FICTITIOUS CALCULATION EXAMPLE−0.5 K±0+0.5 K0102030405060Time in minutesNetwork flow± 0.5 K, period 10 minInstrument inletafter buffer, τ = 20 min± 0.04 Kresidual fluctuationat the instrument (steady state)τ = volume / flow rate,e.g. 100 l at 300 l/h
The buffer volume smooths out fluctuations from the network Fictitious calculation example with assumed values

−92 %less temperature fluctuation at the instrument in the fictitious example with a time constant of 20 minutes

In addition, there is a separate control stage for each instrument, so that faults or the shutdown of one microscope do not affect the others. The network temperature is often overlooked: if the flow temperature of the chilled water network is only slightly below the instrument’s set point, more water has to be mixed in, the control valve works within a usable stroke range and control becomes smoother. Colder is not better here.

05What you should clarify for your project

  • Obtain the installation requirements of each instrument early: heat dissipation to water and room, flow temperature, stability, water quality
  • For every tolerance, check whether a band or drift over time is meant
  • Provide temperature sensors at the instrument inlet with suitable measuring accuracy and recording – as evidence at acceptance
  • Design the pipe network so that later operation via dedicated chiller units remains possible
  • Plan for redundancy, maintenance windows, vibration and magnetic stray fields from the outset

In this way, a supposedly small cooling task becomes a system that enables undisturbed measurements over days.

Takeaway

When cooling cryo-electron microscopes, constancy is the task, not capacity – and constancy is achieved most economically with inertia rather than with ever faster control loops.

Standards and sources

  • Sader et al. (2020): Industrial cryo-EM facility setup and management. Acta Crystallographica Section D 76
  • Meng et al. (2023): Best practice – setting up and operating a mid-sized cryo-EM facility. Frontiers in Molecular Biosciences
  • NIH Office of Research Facilities – Design Requirements Manual, News to Use: Facility Design Criteria for Electron Microscopes (2013)
  • EN IEC 60751 – Industrial platinum resistance thermometers and platinum temperature sensors
  • SIA 384/1 – Heating systems in buildings (basic hydraulic circuits)

SEDC AG · Article from our internal training series “Technik Praxis”, abridged for clients and users.

Full version & expert discussion

More depth for your project.

The full version contains the derivation of volume flow, valve authority and buffer time constant, the hydraulic schematic with control concept, the comparison between direct cooling and cooling via a chiller unit, and our checklist for planning and acceptance. We are happy to go through it with you – applied to your installation.

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