Drop Formation Waveforms for Crosstalk Reduction

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Solution Overview

Problem

In continuous inkjet printing systems, the formation of large drops is often incomplete before reaching the deflection air flow, leading to unintended merging with small drops and neighboring jets, causing disturbances and affecting print quality due to acoustic stimulation crosstalk and uneven drop spacing.

Innovation Solution

A method involving specific drop waveforms with a small drop waveform period approximately equal to the Rayleigh frequency and a large drop waveform with a second pulse occurring within a specific time frame of a subsequent small or large drop waveform, reducing drop formation length and minimizing disturbance to neighboring jets.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Volume of moving object

If a large drop waveform with period Nx is used to form large-volume drops, then the drop volume is increased, but the drop formation length increases causing incomplete coalescence before deflection

Engineering Contradiction:
Improvedrop volumeVSAvoiddrop formation length
Core Design Contradiction:
Volume of moving objectVSLength of moving object

Solution Approach 1:

The large drop waveform is segmented into multiple pulses within the period Nx. The first pulse initiates drop formation and the second pulse completes coalescence, dividing the drop formation process into distinct stages that occur within a shortened overall formation length

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The waveform uses periodic pulsing with period Nx where N is an integer. This periodic action creates controlled disturbances at regular intervals, enabling systematic manipulation of drop formation timing and location to achieve complete coalescence within a reduced formation length

Inventive Principle:
Principle #19Periodic action

2Length of moving object

If the drop formation length is reduced to enable earlier size separation, then the print head size is reduced, but the large drops may not fully coalesce before deflection

Engineering Contradiction:
Improvedrop formation lengthVSAvoidcoalescence completeness
Core Design Contradiction:
Length of moving objectVSReliability

Solution Approach 1:

The first pulse of the large drop waveform initiates drop formation in advance, creating an initial disturbance that begins the coalescence process early. This preliminary action allows the drop formation to start before the drop reaches the deflection region, ensuring complete coalescence within the reduced formation length

Inventive Principle:
Principle #10Preliminary action

Solution Approach 2:

The second pulse in the large drop waveform acts as a feedback mechanism that monitors and completes the coalescence process. By applying a second pulse within the period Nx, the system ensures that any incomplete coalescence is corrected, guaranteeing complete drop formation before deflection

Inventive Principle:
Principle #23Feedback

3Manufacturing precision

If small-volume drops are produced with period x at Rayleigh frequency, then the drop spacing is controlled, but uneven spacing and unintended merging with large drops occurs

Engineering Contradiction:
Improvedrop spacing uniformityVSAvoidacoustic stimulation crosstalk
Core Design Contradiction:
Manufacturing precisionVSObject-generated harmful factors

Solution Approach 1:

The system changes the waveform parameters (period, pulse width, amplitude) depending on the desired drop volume. Small drops use period x at Rayleigh frequency while large drops use period Nx with multiple pulses. This parameter adjustment controls drop spacing and minimizes acoustic stimulation crosstalk between neighboring jets

Inventive Principle:
Principle #35Parameter changes

Solution Approach 2:

Each jet in the nozzle array is assigned a specific waveform pattern tailored to its function. Jets producing small drops receive one waveform while jets producing large drops receive a different waveform. This local customization ensures optimal drop spacing and minimizes harmful acoustic interactions between adjacent jets

Inventive Principle:
Principle #3Local quality

Applied Scientific Principles

This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.

Function Achieved in This Case

This approach ensures complete coalescence of large drops before deflection, reduces drop formation length, and minimizes disturbances to neighboring jets, enhancing print quality and reducing the risk of incomplete or merged drops.

Implementation Method 1

periodic heat pulses drive capillary break-up of jets formed at each nozzle to produce an array of drops

Methodology Applied
Scientific EffectCapillary break-up: Plateau-Rayleigh Instability

Implementation Method 2

the jet responds most sensitively to disturbances at a characteristic frequency fR known as the Rayleigh frequency

Methodology Applied
Scientific EffectRayleigh frequency: Resonance

Implementation Method 3

A gas flow directed across the stream of ink drops interacts with the stream of ink drops. This interaction deflects smaller drops more than larger drops

Methodology Applied
Scientific EffectGas flow deflection: Drag

Data Source

PatentUS8684483B2Drop formation with reduced stimulation crosstalk
Publication Date: 2014.04.01 EASTMAN KODAK CO
  • US8684483B2 patent drawing
  • US8684483B2 patent drawing
  • US8684483B2 patent drawing

AI summary

A liquid stream is caused to jet from a nozzle. A small or large drop waveform applied to a drop forming mechanism causes the liquid stream to break up into a small or large volume drop, respectively. The small drop waveform includes a pulse having a width wS, and a period x, where x≈1/fR, where fR is the Rayleigh frequency of the liquid. The large drop waveform includes a period Nx, with the large volume drop being N times the small volume drop. The large drop waveform includes a first pulse having a pulse width wL1, where wL1≧wS, and a second pulse occurring within a period of (fR/fC)x of an initial pulse of a subsequent small or large drop waveform, where fC is the cut off frequency of the liquid. The second pulse includes a pulse width wL2, where wL2<wS.