Hawkins Electrical Guide v. 03 (of 10): Questions, Answers, & Illustrations, A progressive course of study for engineers, electricians, students and those desiring to acquire a working knowledge of electricity and its applicationsHawkins, N. (Nehemiah)
Science
Hawkins Electrical Guide v. 03 (of 10): Questions, Answers, & Illustrations, A progressive course of study for engineers, electricians, students and those desiring to acquire a working knowledge of electricity and its applications
Hawkins, N. (Nehemiah)
Electrical engineering -- Handbooks, manuals, etc.
[Illustration: Fig. 557.--Differential galvanometer method of testing
resistances. In making the test, the resistance box is adjusted till the
galvanometer needle shows no deflection. When this condition obtains,
the resistance in circuit in the resistance box is equal to the unknown
resistance, hence, a reading of the box gives the value of the unknown
resistance.]
Ques. What name is given to this method of testing?
Ans. It is called a _zero_ method, distinguishing it from _deflection_
methods.
Ques. For what kind of resistance is the method adapted?
Ans. Since it is a nil or zero method, it is better adapted to the
measurement of non-inductive than of inductive resistances.
Ques. What precaution should be taken with inductive resistances?
Ans. The current must be allowed to flow until it becomes steady to
overcome the influence of self-induction.
Ques. What may be said with respect to the differential galvanometer
method?
Ans. With an accurate instrument it is very reliable.
[Illustration: Fig. 558.--Drop method of testing resistances. The
apparatus is connected as shown and readings taken with voltmeter across
known and unknown resistance. The unknown resistance is then easily
calculated.]
Drop Method.--This is a convenient method, and one which may be used for
measuring either high or low resistances with precision. It is used for
many practical measurements, and requires only a voltmeter, battery, known
resistance and a two way switch.
The instruments are connected as in fig. 558, and in making the test,
the voltmeter is switched into circuit across the known resistance and
then across the unknown resistance, readings being taken in each case.
The value of the unknown resistance, is then easily calculated from the
following proportion:
drop across known resistance known resistance
------------------------------ = ------------------
drop across unknown resistance unknown resistance
from which
unknown known resistance × drop across unknown resistance
resistance = ---------------------------------------------------------
drop across known resistance
Public-domain text, read in full here on John Shaqi.
Reviews
Reviews
No reviews yet
Be the first to share your thoughts on this work.
Join the Discussion
Join the discussion
Sign in to leave a comment or review.
Sign InorCreate an account