Respuesta :
It depends on how the polarities of the two batteries are placed.
Here I assume that the battery on the left side has polarity- on top and polarity-+on bottom, while the battery on the right side has polarity- on bottom and polarity+ on top, so the current is flowing in anti-clockwise direction.
To solve the problem, we must first calculate the current flowing in the circuit. For this, we use Kirchoff's voltage law:
[tex]\sum V_i =0[/tex] (1)
We must consider both the emf of the batteries and the voltage drops on the resistors, which for sign convention we must take as negative. So (1) becomes
[tex]15 V - (1 \Omega \cdot I)+5 V -(4 \Omega \cdot I)=0[/tex]
where I is the current flowing.
By solving the equation, we get:
[tex]20 V=5 I[/tex]
[tex]I= 4 A[/tex]
So, assuming the potential at top left corner is 0 V (because it is at same potential of the negative polarity of the 15 V battery), then the voltage drop on the [tex]4 \Omega[/tex] resistor is [tex]\Delta V = IR=(4 A)(4 \Omega)=16 V[/tex], and so the potential at the top right corner is 16 V. Instead, the bottom left corner is at same potential of the positive terminal of the 15 V battery, so at 15 V.
In case the polarities of the 5 V battery are inverted, the exercise must be re-done in the same way by changing the sign of the emf of the 5 V battery in the Kirchoff's law.
Here I assume that the battery on the left side has polarity- on top and polarity-+on bottom, while the battery on the right side has polarity- on bottom and polarity+ on top, so the current is flowing in anti-clockwise direction.
To solve the problem, we must first calculate the current flowing in the circuit. For this, we use Kirchoff's voltage law:
[tex]\sum V_i =0[/tex] (1)
We must consider both the emf of the batteries and the voltage drops on the resistors, which for sign convention we must take as negative. So (1) becomes
[tex]15 V - (1 \Omega \cdot I)+5 V -(4 \Omega \cdot I)=0[/tex]
where I is the current flowing.
By solving the equation, we get:
[tex]20 V=5 I[/tex]
[tex]I= 4 A[/tex]
So, assuming the potential at top left corner is 0 V (because it is at same potential of the negative polarity of the 15 V battery), then the voltage drop on the [tex]4 \Omega[/tex] resistor is [tex]\Delta V = IR=(4 A)(4 \Omega)=16 V[/tex], and so the potential at the top right corner is 16 V. Instead, the bottom left corner is at same potential of the positive terminal of the 15 V battery, so at 15 V.
In case the polarities of the 5 V battery are inverted, the exercise must be re-done in the same way by changing the sign of the emf of the 5 V battery in the Kirchoff's law.
(a) The potential at the upper right of the square is 13.32 V.
(b) The potential at the lower left corner of the square is 3.33 V.
Net voltage in the circuit
The net voltage in the circuit is determined by applying Kirchhoff rule assuming the current flow is anticlockwise.
∑V = 0
Assuming the following
- Top of the square = positive
- Bottom of the square = negative
- Right of the square = positive
- Left of the square = negative
-15 + (4I) + 5 - (1I) = 0
-10 + 3I = 0
3I = 10
I = 10/3 = 3.33 A
Potential at the upper right = 3.33 x 4 = 13.32 V
Potential at the lower left corner = 1 x 3.33 = 3.33 V.
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