Short Name: 
CN, CPC
HAIS Instrument: 
No

Manufacturer or Builder:

Deployments: 
WE-CAN
SOCRATES
ARISTO 2016
ORCAS
ARISTO 2015
CSET
SABIRPOD
WINTER
FRAPPE
NOMADSS
DC3
TORERO
IDEAS-4_C130
ICE-T
DC-3 TEST
WAMO/ICARE
PLOWS
VOCALS
ICE-L
PASE
ACME
GOTEX
EPIC
DYCOMS-II
MAP
Date Acquired: 
September, 1988
Current Location: 

RAF

Property Tag and/or Serial Number: 
PPE17703 (C-130 3760A), PPE17704 (3760A), PPE15447 (3010S), PPE11690 (WCPC S/N 132), PPE11708 (WCPC S/N 133)
Operational Status: 
requestable, ready for deployment
Model: 
TSI-3760A (others: TSI-3010S, WCPC-LP)
Lead Contact: 
Mike Reeves
Alternate Contact: 
Jorgen Jensen
Measurements Provided: 
The total ambient concentration of aerosol particles larger than the threshold size for the instrument, typically about 11 nm diameter (6 nm for the water-based counter), but dependent on flight conditions.
Typical Sampling Rates: 
10 Hz
General Description: 
  • *** As of 2016, the water-based CPCs (WCPC-LP) are no longer requestable ***
  •  
  • Photograph of the 3760A butanol-based CN counter:
  • Condensation nuclei are particles that serve as condensation centers when exposed to high supersaturations of some condensible vapor such as butanol or water.  They are normally detected by exposing the airstream to such a supersaturated vapor and then detecting the resulting droplets after they grow to sizes where they are readily counted by, e.g., an optical counter.  The supersaturation used is typically about 300%.

  • Currently the only condensation nucleus counter in use by RAF is a butanol-based TSI 3760A packaged with a pump, pressure gauge, temperature sensor, and mass flow meter.  A modified version of a TSI 3786 ultra-fine water-based CN counter, which has flown in the past, is no longer requestable.  Because the 3760A counting efficiency drops rapidly with pressure below about 250 mb, it is unsuitable for high-altitude measurements aboard the NCAR/NSF GV.

  • Particles flow continuously through a small internal chamber where they are counted, and concentrations are then determined by dividing by the volume flow rate.  RAF data processing then converts the measured instrument concentration to equivalent ambient concentration (not to standard conditions).  The threshold (50% efficiency) particle size detected by the butanol instrument is about 11 nm, although this varies somewhat with pressure.  The data processing also includes a correction for particle coincidence in the detection volume, which becomes increasingly important as particle concentration increases.  With this correction, the instrument continues to perform with uncertainty < 10% up to concentrations around 10,000 cm-3.  Tubing losses can be significant for small particles, and size-dependent and pressure-dependent errors may become significant unless the lines can be kept very short.

  • Sources of CN in the atmosphere include combustion by-products (soot), wind-generated dust, sea spray salt, gas-to-particle reactions, residues from in-cloud aqueous chemical reactions, etc.  Atmospheric removal of CN occurs primarily through growth to larger sizes by coagulation with other particles, gravitational or inertial settling, and (dominantly) scavenging by clouds.  Typical concentrations of CN are ~100 cm-3 in clean background air and ~5,000 cm-3 in cities, with peak values > 50,000 cm-3.

History of Significant Changes: 
  • 2014:  Corrected the algorithm for coincidence correction.  The previous correction was specific to an older model TSI CNC, and had been applied improperly for many years.
  • 2015:  Corrected erroneous calibration coefficients for both sample flow and bypass flow meters.  Previous calibrations had been in use for years.

 

Time series of CN ambient concentration (blue) along with UHSAS-A total concentration (red) for RF04 in SOCRATES.  Geometric altitude (green, r.h. axis) is also plotted: