Leon Charles Thevenin was born in Paris on March 30th 1857.
He graduated from the Ecole Polytechnique in 1876 and two years later
joined the Corps of Telegraph Engineers. Appointed as a teaching inspector at
the École supérieure de télégraphie in 1882, he was interested in the problems
of measurement in electrical circuits. As a result of studying Kirchhoff's
circuit laws and Ohm's law, he developed his famous theorem, Thévenin's
theorem, which made it possible to calculate currents in more complex
electrical circuits and allowing people to reduce complex circuits into simpler
circuits, called Thévenin's equivalent circuits. His Theorem was published in
three separate scientific journals in 1883 in a paper entitled "Extension
of Ohm's Law to complex electrical circuits". Three more articles followed
in that year. The first gave a method of using a galvanometer to measure
potential, and made use of the new theorem. The second described a method for
measuring resistance, and the third was on the use of the Wheatstone Bridge.
He was described as a humble man, a model engineer and a kind hearted
person. He died on 21st September 1926 in Paris. He lived for 69
years on this planet and even today he lives in every basic electrical and
electronics textbooks.
THEVENIN’S THEOREM
Any linear active
bilateral network can be replaced by an equivalent circuit consisting of
voltage source in series with a resistance. The voltage source is open circuit
voltage across the open circuited load terminals and the resistance being the
internal resistance of the source network looking from the open circuited load
terminals.
[OR]
Any
two terminal linear network, containing independent voltage and current
sources, may be replaced by a constant voltage source VTH
in series with a resistance RTH where VTH
is the open circuit voltage between the terminals and RTH is the
resistance of the network as seen from the two terminal with all sources
replaced by their internal resistances.
APPLICATIONS
1. This theorem is extensively
used in networks to determine the current through any element or voltage across
any element in a network without rigorous calculation for solving a set of
network equations.
2. It is useful in
circuit analysis when it necessary to find the current only in one branch of a
circuit.
3. It is also useful
when it is necessary to study the variation in the current in a branch of the
circuit when the resistances of this branch is varied.
No comments:
Post a Comment