Voltage Sources in Parallel
Introduction
In electrical and electronic circuits, voltage sources are used to provide electrical energy to loads. In many practical applications, more than one voltage source is connected together to improve reliability or current capacity. One such configuration is voltage sources connected in parallel. Understanding how voltage sources behave when connected in parallel is important for circuit design, power systems, and electronics.What Are Voltage Sources in Parallel?
Voltage sources are said to be connected in parallel when their positive terminals are connected together and their negative terminals are connected together, supplying power to a common load. In this arrangement:Ideal Voltage Sources in Parallel
Important RuleCondition for Parallel Connection
For ideal voltage sources to be connected in parallel: All sources must have exactly the same voltage magnitude and polarity.Practical Voltage Sources in Parallel
In real-life circuits, voltage sources are not ideal. Each practical voltage source has a small internal resistance (r). When voltage sources with internal resistance are connected in parallel: This makes parallel connection possible and safe in practical systems such as batteries and power supplies.Equivalent Voltage Source in Parallel
For n identical voltage sources connected in parallel: Equivalent Voltage (Vₑq) $$ V_{eq} = V $$ Equivalent Internal Resistance (rₑq) $$ \frac{1}{r_{eq}} = \frac{1}{r_1} + \frac{1}{r_2} + \cdots + \frac{1}{r_n} $$ If all internal resistances are equal: $$ r_{eq} = \frac{r}{n} $$ This shows that connecting voltage sources in parallel reduces internal resistance, allowing the system to deliver more current.Current Sharing in Parallel Voltage Sources
The total load current is divided among the sources based on their internal resistances. For two sources: $$ I_1 = \frac{r_2}{r_1 + r_2} I_{total} $$ $$ I_2 = \frac{r_1}{r_1 + r_2} I_{total} $$ Where: ($I_1$, $I_2$) = currents from each source ($r_1$, $r_2$) = internal resistances A source with lower internal resistance supplies more current.
Example 1: Two Batteries in Parallel
Given:
-
Battery 1: ($V = 12V$), ($r_1 = 0.2Ω$)
Battery 2: ($V = 12V$), ($r_2 = 0.2Ω$)
Load resistance ($R_L = 6Ω$)
Advantages of Voltage Sources in Parallel
✔ Increased current capacity✔ Improved reliability (backup operation)
✔ Reduced internal resistance
✔ Longer battery life in battery systems
Disadvantages
✖ Circulating currents if voltages are mismatched✖ Unequal current sharing if internal resistances differ
✖ Requires careful design and protection
Practical Applications
Voltage sources in parallel are widely used in:- Battery banks (UPS systems, solar systems)
- DC power supplies
- Electric vehicles
- Telecommunication power systems
- Redundant power systems in industries
Conclusion
Voltage sources connected in parallel provide the same output voltage while increasing the available current capacity. This configuration is widely used in practical power systems where reliability and higher current delivery are required. However, proper design is essential to avoid circulating currents and ensure safe operation.Why we need Parallel Voltage Sources
The primary reason for placing two or more batteries or supplies in parallel is to increase the current rating above that of a single supply. For example, in Fig. 1, two ideal batteries of 12 V have been placed in parallel. The total source current using Kirchhoff's current law is now the sum of the rated currents of each supply. The resulting power available will be twice that of a single supply if the rated supply current of each is the same. That is,with $I_1 = I_2 = I$ then
$$P_T = E(I_1 + I_2)$$
$$= E(I + I) = E(2I) $$
$$= 2(EI) = 2P$$
Fig. 1: Examining the impact of placing two lead-acid
batteries of different terminal voltages in parallel.
Fig. 2: Examining the impact of placing two lead-acid batteries of different terminal voltages in parallel.
$$ I = {E_1 - E_2 \over R_{int1} + R_{int2}}$$
$$= {12 V - 6 V \over 0.03 Ω + 0.02 Ω}$$
$$ = {6 V \over 0.05 Ω} = 120 A$$
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