Use nodal analysis to solve the circuit and determine the values of and
.

I. Identify all nodes in the circuit.
There are four nodes in the circuit:

II. Select a reference node.
There is symmetry in this circuit and each node has three elements connected to. One of the elements connected to each node is a voltage source. Thus, any node has no advantage over others in being the reference node. We choose the bottom left node as the reference node.

III. Assign variables for unknown node voltages.
Three remaining nodes are labeled as shown in the figure above. With this labeling, the value of can be determined directly. Since there is a voltage source between the node of
and the reference node, and the positive terminal of the voltage source is connected to the reference node, we have:
The label is assigned to simplify referencing this node in the analysis. Alternatively, one could avoid assigning a label to this node and instead directly substitute
wherever it is required in the equations.
IV. Incorporate dependent sources.
This circuit does not contain any dependent sources.
V. Apply Kirchhoff’s Current Law (KCL).
We write a single KCL equation for the super-node:
Multiplying by 20
(1)
VI. Handle super-nodes.
Nodes and
are connected by a voltage source, forming a super-node. By applying Kirchhoff’s Voltage Law (KVL) to the loop shown below,
can be expressed in terms of
as follows:

(2)
VII. Solve the System of Equations.
Substituting (2) in (1):
Substituting and the known values into the equation, we solve for
:
At this point, the circuit is fully solved, and all node voltages are determined.
VIII. Determine Additional Variables. Calculating and
With the node voltages known, we can now calculate and
.
KCL at Node 1:
KVL around the loop shown below

Download the Circuit File
To download the LTspice circuit file for your own simulations, click the link below.Please remember to unzip the file after downloading to access the .asc file for your simulations:

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