Concept:
When electrical components are connected in
parallel, they are all connected between the same two nodes (junction points) of the circuit. This is the defining characteristic of a parallel connection --- all components share the same two terminals, and therefore the same potential difference (voltage) appears across each of them.
Step 1: Understand parallel connection geometrically.
In a parallel circuit, if we have resistors $R_1$, $R_2$, $R_3$ connected in parallel between nodes A and B:
• One end of every resistor is connected to node A.
• The other end of every resistor is connected to node B.
• The voltage from A to B is fixed (let's call it $V$).
• Therefore, the potential difference across $R_1$ = potential difference across $R_2$ = potential difference across $R_3$ = $V$.
Step 2: Recall the two basic circuit laws.
Kirchhoff's Voltage Law (KVL): The sum of potential differences around any closed loop is zero. In a parallel branch, each branch forms a separate closed loop with the source, and each loop has the same source voltage across it.
Result: $V_{R_1} = V_{R_2} = V_{R_3} = V$ (the supply voltage).
Step 3: Note the contrast with series connection.
tabular|l|l|l|
Property &
Series &
Parallel
Voltage &
Different (split) &
Same (equal for all)
Current & Same through all & Different (splits)
tabular
Step 4: Check the wrong options.
• (A) Different: Voltage being different across resistors is the characteristic of a series circuit, not parallel.
• (C) Zero: If voltage were zero across resistors, no current would flow. This is only true for ideal short circuits.
• (D) Double: There is no doubling of voltage in a parallel resistor connection. Voltage stays equal to the supply.