Dynamics of field-induced droplet ionization: time-resolved studies of distortion, jetting, and progeny formation from charged and neutral methanol droplets exposed to strong electric fields.

The journal of physical chemistry. B · 2005 · Unclear · Insufficient evidence

← Research stream
UnclearInsufficient evidencePaper 3571

Using switched high electric fields, 225 µm methanol droplets (neutral and charged) were observed to distort and form Taylor cone-jets, emitting ~10 µm charged progeny droplets at a critical field strength. Neutral droplets formed symmetric cone-jets of both …

Study snapshot

PublicationThe journal of physical chemistry. B · 2005
Study typeother
Reported directionUnclear
Evidence ratingInsufficient

Abstract

We recently reported that strong electric fields may be employed to directly extract positive and negative ions for mass analysis, including intact proteins, from neutral droplets. The present study investigates the dynamics of this process using switched high electric fields to enable time-resolved studies of droplet distortion, Taylor cone formation, and charged progeny droplet extraction from neutral and charged 225 microm methanol droplets. After a specific time in the field, a flashlamp is triggered to record droplet distortions using shadow photography. At a critical field strength E(c)0 corresponding to the Taylor limit, neutral droplets exhibit a prolate elongation along the field axis forming symmetric cone-jets of positive and negatively charged progeny droplets, approximately 10 microm in diameter. This process is termed field-induced droplet ionization (FIDI). Because the time scale of FIDI is related to the frequency of shape oscillations that occur below the Taylor limit, models of field-dependent oscillation become an important predictor of the time scale for progeny jet formation. Droplets with a net charge q distort into asymmetric tear shapes and emit a single charged jet of progeny at a critical field E(c)(q) that is less than E(c)0. The measured decrease in droplet stream charge indicates that total charge loss can be greater than the original charge on the droplet, resulting in oppositely charged droplets. Interestingly, above E(c)0, charged droplets sequentially emit a jet of the same polarity as the net charge followed by a jet of reverse polarity emitted in the opposite direction. For both neutral and charged droplets, increasing the electric field decreases the time to form jets and the combination of net charge and higher-than-critical fields has a compound effect in accelerating progeny formation. The implications of our results for using switched fields in FIDI-mass spectrometry for on-demand ion sampling from neutral and charged droplets are discussed.

Machine Enhanced Logic

AI evidence extraction

Structured fields below were generated from the paper’s abstract and metadata to make the evidence easier to inspect. Automated extraction may be incomplete or incorrect; verify important details against the original paper.

Study typeother
Effect directionunclear
PopulationNot supplied
Sample sizeNot supplied
ExposureNot supplied
Evidence strengthInsufficientConfidence: 74% · Peer reviewed: yes

Main findings

Using switched high electric fields, 225 µm methanol droplets (neutral and charged) were observed to distort and form Taylor cone-jets, emitting ~10 µm charged progeny droplets at a critical field strength. Neutral droplets formed symmetric cone-jets of both polarities at a critical field corresponding to the Taylor limit, while charged droplets distorted asymmetrically and emitted a single charged jet at a lower critical field; above the neutral-droplet critical field, charged droplets could emit sequential jets of opposite polarity. Increasing electric field strength reduced the time to jet formation, and net charge plus higher-than-critical fields further accelerated progeny formation.

Outcomes measured

  • Droplet distortion/elongation
  • Taylor cone formation
  • Jetting and progeny droplet formation
  • Charge loss and polarity of emitted jets
  • Time to jet/progeny formation as a function of field strength and net charge
View raw extracted JSON
{
  "study_type": "other",
  "exposure": {
    "band": null,
    "source": "strong electric fields (laboratory)",
    "frequency_mhz": null,
    "sar_wkg": null,
    "duration": null
  },
  "population": null,
  "sample_size": null,
  "outcomes": [
    "Droplet distortion/elongation",
    "Taylor cone formation",
    "Jetting and progeny droplet formation",
    "Charge loss and polarity of emitted jets",
    "Time to jet/progeny formation as a function of field strength and net charge"
  ],
  "main_findings": "Using switched high electric fields, 225 µm methanol droplets (neutral and charged) were observed to distort and form Taylor cone-jets, emitting ~10 µm charged progeny droplets at a critical field strength. Neutral droplets formed symmetric cone-jets of both polarities at a critical field corresponding to the Taylor limit, while charged droplets distorted asymmetrically and emitted a single charged jet at a lower critical field; above the neutral-droplet critical field, charged droplets could emit sequential jets of opposite polarity. Increasing electric field strength reduced the time to jet formation, and net charge plus higher-than-critical fields further accelerated progeny formation.",
  "effect_direction": "unclear",
  "limitations": [],
  "evidence_strength": "insufficient",
  "confidence": 0.74,
  "peer_reviewed_likely": "yes",
  "keywords": [
    "electric fields",
    "field-induced droplet ionization (FIDI)",
    "methanol droplets",
    "Taylor cone",
    "jetting",
    "progeny droplets",
    "shadow photography",
    "time-resolved"
  ],
  "suggested_hubs": [
    {
      "slug": "engineering",
      "weight": 0.6,
      "reason": "Laboratory study of strong electric-field effects on droplet ionization/jetting relevant to instrumentation (FIDI mass spectrometry)."
    }
  ]
}
AI can be wrong. Always verify against the paper.

AI-extracted fields are generated from the abstract and metadata and may be incomplete or incorrect. This material is for informational purposes and is not medical advice.

Identifiers and source

DOI: 10.1021/jp0450540
PubMed: 16851963

Read the original paper →

Related papers

← Back to the Research Library