Update on results at Coolescence, LLC

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Presentation transcript:

Update on results at Coolescence, LLC Rick Cantwell Coolescence, LLC Boulder, CO rick@coolescence.com +1 720-565-9690 October 2008

Coolescence, LLC Founded in 2005, Angel funded, 3 researchers Areas of experiments Calorimetry Glow Discharge initiated LENR Built on work of Karabut & Energetics Initial goal to measure excess heat with calorimeter -2 generations of calorimeter – will discuss 2nd generation. No positive excess heat results from GD work yet. Will discuss loading data October 2008

Calorimeter for GD Experiment Flow Calorimeter surrounding vacuum chamber (320 cm3) Cathode Pt RTD allows Isoperibolic operation Built-in Joule Heater Goal to build put a flow calorimeter around a small vacuum chamber – work over 10W with 1% error During operation saw that isoperibolic operation also possible and more accurate Chamber open – note screw in cathode, heaters Assembled chamber – note HV anode wire Chamber with rear heat capture block October 2008

Calorimeter Engineering Dual In/Out temp measurement (thermistor) 2 stage fluid temp regulation (+/-5 mDegC) Air temp regulation (+/- 50 mDegC) Fluid temp regulated with standard recirculating chiller + software controlled Peltier heater/cooler Air temp regulated with software controlled Peltier heater/cooler Chamber surronded by both heat transfer pieces (Aluminum) Heat transfer blocks surronded by insulation Entire assembly surronded by constant temp box October 2008

Daul Calorimeter Block Diagram Built as two similar units side by side – allows for direct comparison of control parts constant volume pump 2nd stage input temp polish cool fluid back to original temp for 2nd chamber controlled by LabView program Agilent 34970 6-1/2 digit data acquisition October 2008

Calorimeter Performance Flow Calorimeter Sensitivity: 20mW Capture Ratio: 90-94% Time constant: 19 minutes Isoperibolic Calorimeter Sensitivity: 5mW Time constant: 5 minutes Sensitive to pressure, heat location Flow calorimeter has ~2% variation based on location/type of heat, slow Isoperibolic – more sensitive – very large variations based on heat location, pressure, gas type October 2008

Typical Performance Isoperibolic used different calibration constants for glow or heater No calibration constant used for flow calorimeter (just zeroed) October 2008

Glow Discharge Loading of Pd Initial focus on Glow Discharge initiated LENR using calorimetry to find anomalous heat No excess heat results Characterize deuterium loading with Glow Discharge October 2008

Apparatus & Techniques .3 & 1.5 liter chambers Glow in 1-10 torr D2 Pd foils (25-100 micron) attached with diffusion weld Pd & Pd alloy thin films (1-5 micron) on copper Loading measured by gas loss (pressure drop) Verify by pressure rise during unloading Capacitive Manometers Use standard cathode 1.2” Cu disk Screws into holder – can cool with water Test foils welded – also tried screws, adhesive- Baratron gauges – fast, gas insensitive Example of sputtered disks – provided by Colorado School of Mines – research agreement October 2008

Major Loading Observations No high loading (D/Pd < .7) No bulk loading at higher temperatures Loading rate proportional to current (J<100mA/cm2) 5-10 D’s loaded for each D+ of ion current (Faradaic Efficiency 5-10) High D flux during pulsed discharge (.01 sccm/cm2 per mA of glow) Loading rate insensitive to temperature, voltage, and pressure GD causes damage to Pd (sputtering) No loading above .7 Temps’s > ~80 deg C part Pd will unload at 5-10 torr – but will still load on surface Loading rate appears insensitive to temperature, voltage, & pressure (most work on temperature) High D flux - @100 mA glow flow is 1sccm – same as Iwamura work October 2008

Loading Efficiency vs. D/Pd Faradaic Efficiency: defined as number of D’s removed from chamber for each electron of current flow Characteristics: Starts loading typically starts slower, flat area, then falls off. down spikes where gas added. Note: pink curve – stopped loading when glow off, unload when glow off, re-start with higher FE, then quickly falls off. October 2008

Pulsed Glow Discharge Pulse GD technique – appears useful in understanding loading behavior Pulse GD – typical waveform with 4 regions yellow – pulse on – pressure rise from heating light blue – loading – pressure drop – slope is proportional to loading rate green – pulse off – pressure drop from cooling pink – off period – unloading – slope is proportional to unloading rate – unloaded part this is flat When bulk is loading get overall downward slope – flat in the off region When bulk is unloading get overall upward slope – unloads more in off period than is loaded in on period October 2008

Loading vs. Glow Current Example of pulsed loading data Use slope to measure loading rate – Loading rate is proportional to glow current Note doted pink turn around in the pressure – part is starting to unload during the glow October 2008

Loading Rate & Temperature Loading vs Temp Sample 40 12 10 8 6 Faradaic Efficiency 4 Not much sensitivity to temperature in loading rate with short pulses. Note: we don’t see bulk loading at higher temperatures – so this is a surface phenomena Difference between higher and lower current is probably related to some glow escaping the region around the Pd cathode 2 20 40 60 80 100 120 140 160 Temp 2.5 mA 10 mA 25 mA 50 mA 5ma October 2008

Physical Effects of GD 400x optical magnification Significant sputtering of the Pd cathode is observed Any special treatment on surface is rapidly sputtered away October 2008

Questions raised by GD loading results What is mechanism of loading? What limits loading to D/Pd ~ .7? Are common mechanisms at work in GD (Karabut, Savvitamova, Energetics, …), gas flow (Li) and gas flow transmutation (Iwamura)? Was high loading present in earlier GD and gas flow experiments? Last question – is motivating our work Loading is not wholly due to ions. Do incoming ions that cause sputtering also “shake” D out of the lattice? This works suggests that high bulk loading is probably not involved in Karabut, Li, Iwamura experiments. October 2008

Acknowledgements Scott Little Ed Storms October 2008