inductance of pair concentric
Posted by
SAQIB SATTAR
Saturday, October 15, 2011
Labels:
equations,
pair concentric inductance,
pair concentric inductance equation,
what is pair concentric inductance
0
comments
Purely inductive a.c. circuits
Posted by
SAQIB SATTAR
Friday, October 14, 2011
Labels:
ac circuit diagram,
crosstalk tutorial,
inductive ac circuit,
inductive circuit,
series ac cricuits
0
comments
Linear and non-linear devices
Posted by
SAQIB SATTAR
Labels:
diagram,
linear device tutorial,
linear devices,
linear vs non linear divices,
types of linear devices,
what is linear device
1 comments
The figure 2.3 shown below is showing a circuit. In this circuit, current I can be varied by making use of the variable resistor R2. For different setting conditions of R2, the current flowing in the resistor R1, displayed onthe ammeter, and the potential difference "p.d"across R1, displayed on the voltmeter, are noted and a graph is plotted of p.d. against the current. Diagram 2.4(a) shows the results where the straight line graph passing through the origin indicates that current is directly proportional to the p.d. Since the gradient, that is, p.d./current, is constant, resistance R1 is constant. A resistor, therefore, is a good example of a linear device.
Series resonance
Posted by
SAQIB SATTAR
Thursday, October 13, 2011
Labels:
graph,
illustration,
series resonance circuits,
tutorial on seres resonance
0
comments