Ionization Potential Set Up, IP-01 Ionization Potential Set Up, IP-01 Ionization Potential Set Up, IP-01 Ionization Potential Set Up, IP-01
Ionization Potential Set Up, IP-01
Ionization Potential Set Up, IP-01 Ionization Potential Set Up, IP-01 Ionization Potential Set Up, IP-01

Ionization Potential Set Up, IP-01

39500.00 - 46600.00 INR/Piece

Product Details:

  • Weight 10 Kg Kilograms (kg)
  • Material Electronics
  • Application Laboratory Experiment
  • Usage Laboratory Experiment
  • Color Grey
  • Supply Ability : 100 Piece Per Month
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Price And Quantity

  • 1 Piece
  • 39500.00 - 46600.00 INR/Piece

Product Specifications

  • Laboratory Experiment
  • Grey
  • Laboratory Experiment
  • Electronics
  • 10 Kg Kilograms (kg)

Trade Information

  • Telegraphic Transfer (T/T), Delivery Point (DP), Cheque, Cash in Advance (CID), Cash Advance (CA), Cash on Delivery (COD), Cash Against Delivery (CAD)
  • 100 Piece Per Month
  • 1 Week
  • Contact us for information regarding our sample policy
  • Africa, Middle East, Western Europe, Eastern Europe, South America, North America, Central America, Australia, Asia
  • All India
  • ISO 9001: 2015 CE

Product Description

We are highly preferred and major manufacturer, supplier and exporter of Ionization Potential Set Up in Roorkee, Uttarakhand, India. The electrons in the atomshave discrete stationary states.Franck and Hertz in 1914 described the first observation of quantized excitation from one quantized state to another one year after N. Bohr published his theory of hydrogen atom. His method depends on detecting the on-set of inelastic collisions between electrons and atoms of the gas under study.

The experimental tube in this measurement is essentially a triode filled with the vapour of the experimental substance. The electrons emitted by the heated filament of the tube are accelerated by the positive potential VGK between the cathode and the grid. The grid is a wire mesh which allows the electrons to pass through. The anode A is maintained at a fixed potential VGA slightly negative with respect to the grid. In the experiment the electron current is measured as a function of the voltage VGK. As VGK increases, the energy of the electrons increases, and more and more electrons reach the anode. The anode current increases. The collisions between the electrons and the atoms are elastic. As VGK further increases, the energy of the electrons reaches the threshold for the excitation of the atomic electrons from the ground state to the first excited state, and the collisions between the electrons and the atoms become inelastic.


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