Step 1: Understanding the Concept:
Ohmic resistances (or conductors) are those that obey Ohm's Law, which states that the current (I) through a conductor is directly proportional to the voltage (V) across it, provided the temperature and other physical conditions remain unchanged (\(V \propto I\)).
Non-ohmic resistances are those that do not obey Ohm's Law. Their V-I relationship is not linear.
Step 2: V-I Graph for Ohmic Resistance:
According to Ohm's Law, \(V = IR\). If R is constant, this is the equation of a straight line passing through the origin, with the slope equal to the resistance R (\( \text{Slope} = \frac{\Delta V}{\Delta I} = R \)). 
Step 3: V-I Graph for Non-Ohmic Resistance:
For non-ohmic devices, the resistance is not constant but changes with voltage or current. The V-I graph is a curve, not a straight line. Examples include semiconductor diodes, transistors, and thermistors. 
Graph Explanation:
Ohmic: A straight line through the origin indicates a constant ratio of V to I, meaning constant resistance.
Non-Ohmic: The curve shows that the ratio of V to I (the resistance) is not constant. The slope of the tangent at any point on the curve gives the dynamic resistance.
Two cells of emf 1V and 2V and internal resistance 2 \( \Omega \) and 1 \( \Omega \), respectively, are connected in series with an external resistance of 6 \( \Omega \). The total current in the circuit is \( I_1 \). Now the same two cells in parallel configuration are connected to the same external resistance. In this case, the total current drawn is \( I_2 \). The value of \( \left( \frac{I_1}{I_2} \right) \) is \( \frac{x}{3} \). The value of x is 1cm.


For the circuit shown above, the equivalent gate is: