CONTENTS.


CHAPTER I.

[§ 1.]Secondary Current by Induction. No Increased E. M. F.Faraday
[2.]Electric Spark and Increased E. M. F. by Induced Current.Page
[3.]Spark in Secondary Increased by Condenser in Primary.Fizeau
[4.]Atmosphere around an Incandescent Live Wire.Vincintini
[5.]Magnetizing Radiations from an Electric Spark.Henry
[6.]Arcing Metals at Low Voltage.Faraday
[7.]Non-arcing Metals at High Voltage. Practical Application.Wurts
[8.]Duration of Spark Measured.Wheatstone
[8a.]Discharge—Intermittent, Constant, and Oscillatory—by Variation of Resistance.Feddersen
[9.]Musical Note by Discharge with Small Ball Electrodes. Invisible Discharge.Faraday
[9a].Pitch of Sound Changed by Approach of Conductor Connected to Earth.Faraday and Mayer
[10.]Brush Discharge. Color. Striæ. Nitrogen Best Transmitter of a Spark, and its Practical Bearing in Atmospheric Lightning. Cathode Brushes in Different Gases.Faraday
[11.]Glow by Discharge. Glow Changed to Spark. Motion of Air. Apparent Continuous Discharge during Glow.Faraday
[12.]Spark. Solids Perforated.Lullin
[13.]Spark. Glass Perforated. Holes Close Together. Practical Application for Porous Glass.Fage
[14] and [14a.]Spark. Penetrating Power. Conducting Power of Gas. Relation of E. M. F. to Pressure of Gases. Discharge through Hydrogen Vacuum Continued with Less Current than that Required to Start it.Knochenhaurer, Boltzmann, Thomson (Kelvin), Maxwell, Varley, Harris, and Masson
[15.]Dust Particles or Rust on the Electrodes Hasten Discharge.Gordon
[16.]Where the Distance is Greater, the Dielectric Strength is Smaller, Both Distances Being Minute.Thomson (Kelvin)
[17.]Discharge through Gases under Very High Pressures. Increased Dielectric Strength.Cailletet
[18.]Discharges in Different Chemical Gases Variably Resisted.Faraday
[19.]Gas as a Conductor. Molecule for Molecule, its Conductivity Greater than that for Gases.Thomson, J. J.
[20.]Relation of Light to Electricity. The Square Root of the Dielectric Capacity Equal to the Refractive Index.Boltzmann, Gibson, Barclay, Hopkinson, and Gladstone
[21.]Hermetically Sealed Discharge Tubes with Platinum Leading-in Wires.Plücker and Geissler
[22.]Luminosity of Discharge Tubes Produced by Rubbing. Increased by Low Temperature.Geissler
[23.]Different Vacua Needed for Luminosity by Friction and by Discharge.Alvergniat
[24.]Phenomena of Discharge around the Edges of an Insulating Sheet.Steinmetz
[25.]Highest Possible Vacuum Considered as a Non-conductor.Morgan
[26.]Constant Potential at the Terminals of a Discharge Tube.De La Rue and Müller
[26a].Polarity of Discharge-tube Terminals in Secondary of Ruhmkorff Coil. Mathematical Deductions.Klingenberg
[27.]Pressure in Discharge Tube Produced by a Spark.Kinnersley, Harris, and Riess

CHAPTER II.

[28.]Actions of Magnetism upon the Arc and Flame.Davy, Bancalari, and Quet
[29.]Rotation of Luminous Discharge by a Magnet. Application in Explaining Aurora Borealis.De La Rive
[30.]Action of Magnet on the Cathode Light. Relations Different according to the Position Relatively to the Magnetic Lines of Force.Plücker and Hittorf
[31.]Discharge Retarded Across, and Accelerated Along, the Lines of Magnetic Force.Thomson, J. J.
[32.]Resistance of Luminosity of the Discharge Afforded by a Thin Diaphragm.Thomson, J. J.
[33.]Forcing Effect of the Striæ at a Perforated Diaphragm.Solomons

CHAPTER III.

[34.]Electric Images.Riess
[35.]Electrographs on Photographic Plate by Discharge.Sanford and McKay
[36.]Positive and Negative Dust Pictures upon Lines Drawn by Electrodes.Lichtenberg
[36a.]Photo-electric Dust Figures.Hammer
[36b.]Dust Portrait.Hammer
[37.]Electrical Images by Discharge Developed by Condensed Moisture.Karsten
[37a.]Magnetographs.McKay
[38.]Bas-relief Facsimiles by Electric Discharge.Piltchikoff
[39.]Distillation of Liquids by Discharge.Gernez
[40.]Striæ. Black Prints on Walls of Tube.De La Rue and Müller

CHAPTER IV.