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chapter 3, problem 41. apply mesh analysis to find ( i ) in fig. 3.87. …

Question

chapter 3, problem 41. apply mesh analysis to find ( i ) in fig. 3.87. circuit diagram with resistors (10ω, 2ω, 4ω, 1ω, 5ω), voltage sources (6v, 8v), and mesh currents ( i_1 ), ( i_2 ), ( i_3 ), and current ( i ) as shown in figure 3.87 for prob. 3.41.

Explanation:

Step1: Define Mesh Currents

Let the mesh currents be \( i_1 \), \( i_2 \), and \( i_3 \) as shown. The current \( i \) is related to the mesh currents by \( i = i_2 - i_3 \) (assuming the direction of \( i \) is upward, so \( i_2 \) flows down through the 1Ω resistor and \( i_3 \) flows up, so the net current is \( i_2 - i_3 \)).

Step2: Write Mesh Equations

Mesh 1 (\( i_1 \)):

The resistors in mesh 1 are 10Ω, 2Ω, and 5Ω? Wait, no. Let's look at the circuit:

  • Mesh 1: 10Ω, 2Ω (shared with mesh 2), and 5Ω (shared with mesh 3)? Wait, no, the circuit has:
  • Mesh 1: 10Ω, 2Ω (left branch), and 5Ω (right branch)? Wait, no, let's re-examine the circuit:
  • The top loop: 10Ω, 6V source (polarity + on left, - on right), 5Ω? Wait, no, the circuit:
  • Top mesh (\( i_1 \)): 10Ω, 6V source (from + to - in the direction of \( i_1 \)), 5Ω? Wait, no, the 2Ω is between mesh 1 and 2, 1Ω is between mesh 2 and 3, 4Ω is in mesh 2, 5Ω is in mesh 3, 10Ω and 6V in mesh 1, 8V in mesh 2 and 3? Wait, maybe better to write KVL for each mesh.
Mesh 1 ( \( i_1 \) ):
  • Resistors: 10Ω (current \( i_1 \)), 2Ω (current \( i_1 - i_2 \), since \( i_1 \) and \( i_2 \) are in opposite directions through 2Ω), and 5Ω (current \( i_1 - i_3 \))? Wait, no, the 6V source: in mesh 1, the voltage source is 6V with + on left, - on right. So KVL:

\( -6 + 10i_1 + 2(i_1 - i_2) + 5(i_1 - i_3) = 0 \)? Wait, no, maybe I messed up the branches. Let's do it properly:

  • Mesh 1: 10Ω (current \( i_1 \)), 2Ω (current \( i_1 - i_2 \), because \( i_1 \) goes right, \( i_2 \) goes left through 2Ω, so net current \( i_1 - i_2 \)), and the 6V source (voltage drop is -6V if we go from + to - in the direction of \( i_1 \)). Wait, no, KVL: sum of voltages around the mesh is zero. Let's take the direction of \( i_1 \) as clockwise. Then:
  • Voltage across 10Ω: \( 10i_1 \) (drop in direction of \( i_1 \))
  • Voltage across 2Ω: \( 2(i_1 - i_2) \) (drop in direction of \( i_1 \), since \( i_1 > i_2 \) or not, but the current through 2Ω is \( i_1 - i_2 \))
  • Voltage across 6V source: -6V (since we go from + to - in the direction of \( i_1 \))
  • Voltage across 5Ω: \( 5(i_1 - i_3) \) (drop in direction of \( i_1 \))

Wait, no, the 5Ω is in the right branch, with current \( i_1 - i_3 \)? Maybe I'm overcomplicating. Let's try again.

Correct Mesh Equations:
  • Mesh 1 ( \( i_1 \) ):
  • Resistors: 10Ω (current \( i_1 \)), 2Ω (current \( i_1 - i_2 \)), 5Ω (current \( i_1 - i_3 \))
  • Voltage source: 6V (polarity + on left, - on right; so in the direction of \( i_1 \), we go from + to -, so voltage drop is -6V)
  • KVL: \( 10i_1 + 2(i_1 - i_2) + 5(i_1 - i_3) - 6 = 0 \)
  • Simplify: \( 10i_1 + 2i_1 - 2i_2 + 5i_1 - 5i_3 - 6 = 0 \) → \( 17i_1 - 2i_2 - 5i_3 = 6 \) ...(1)
  • Mesh 2 ( \( i_2 \) ):
  • Resistors: 2Ω (current \( i_2 - i_1 \)), 4Ω (current \( i_2 \)), 1Ω (current \( i_2 - i_3 \))
  • Voltage source: 8V (polarity + on top, - on bottom; so in the direction of \( i_2 \) (clockwise), we go from - to +, so voltage rise is +8V)
  • KVL: \( -2(i_2 - i_1) + 4i_2 + 1(i_2 - i_3) + 8 = 0 \)
  • Simplify: \( -2i_2 + 2i_1 + 4i_2 + i_2 - i_3 + 8 = 0 \) → \( 2i_1 + 3i_2 - i_3 = -8 \) ...(2)
  • Mesh 3 ( \( i_3 \) ):
  • Resistors: 5Ω (current \( i_3 - i_1 \)), 1Ω (current \( i_3 - i_2 \)), 5Ω? Wait, no, the 5Ω is in mesh 3? Wait, the right branch: 5Ω, 6V source? No, the 5Ω is in mesh 3, and the 1Ω is between mesh 2 and 3, 5Ω in mesh 3, and the 6V source? Wait, no, the 6V source is in mesh 1, 8V in mesh 2 and 3. Let's correct mesh 3:
  • Mesh 3: 5Ω (current \( i_3 - i_1 \)), 1Ω (curren…

Answer:

Step1: Define Mesh Currents

Let the mesh currents be \( i_1 \), \( i_2 \), and \( i_3 \) as shown. The current \( i \) is related to the mesh currents by \( i = i_2 - i_3 \) (assuming the direction of \( i \) is upward, so \( i_2 \) flows down through the 1Ω resistor and \( i_3 \) flows up, so the net current is \( i_2 - i_3 \)).

Step2: Write Mesh Equations

Mesh 1 (\( i_1 \)):

The resistors in mesh 1 are 10Ω, 2Ω, and 5Ω? Wait, no. Let's look at the circuit:

  • Mesh 1: 10Ω, 2Ω (shared with mesh 2), and 5Ω (shared with mesh 3)? Wait, no, the circuit has:
  • Mesh 1: 10Ω, 2Ω (left branch), and 5Ω (right branch)? Wait, no, let's re-examine the circuit:
  • The top loop: 10Ω, 6V source (polarity + on left, - on right), 5Ω? Wait, no, the circuit:
  • Top mesh (\( i_1 \)): 10Ω, 6V source (from + to - in the direction of \( i_1 \)), 5Ω? Wait, no, the 2Ω is between mesh 1 and 2, 1Ω is between mesh 2 and 3, 4Ω is in mesh 2, 5Ω is in mesh 3, 10Ω and 6V in mesh 1, 8V in mesh 2 and 3? Wait, maybe better to write KVL for each mesh.
Mesh 1 ( \( i_1 \) ):
  • Resistors: 10Ω (current \( i_1 \)), 2Ω (current \( i_1 - i_2 \), since \( i_1 \) and \( i_2 \) are in opposite directions through 2Ω), and 5Ω (current \( i_1 - i_3 \))? Wait, no, the 6V source: in mesh 1, the voltage source is 6V with + on left, - on right. So KVL:

\( -6 + 10i_1 + 2(i_1 - i_2) + 5(i_1 - i_3) = 0 \)? Wait, no, maybe I messed up the branches. Let's do it properly:

  • Mesh 1: 10Ω (current \( i_1 \)), 2Ω (current \( i_1 - i_2 \), because \( i_1 \) goes right, \( i_2 \) goes left through 2Ω, so net current \( i_1 - i_2 \)), and the 6V source (voltage drop is -6V if we go from + to - in the direction of \( i_1 \)). Wait, no, KVL: sum of voltages around the mesh is zero. Let's take the direction of \( i_1 \) as clockwise. Then:
  • Voltage across 10Ω: \( 10i_1 \) (drop in direction of \( i_1 \))
  • Voltage across 2Ω: \( 2(i_1 - i_2) \) (drop in direction of \( i_1 \), since \( i_1 > i_2 \) or not, but the current through 2Ω is \( i_1 - i_2 \))
  • Voltage across 6V source: -6V (since we go from + to - in the direction of \( i_1 \))
  • Voltage across 5Ω: \( 5(i_1 - i_3) \) (drop in direction of \( i_1 \))

Wait, no, the 5Ω is in the right branch, with current \( i_1 - i_3 \)? Maybe I'm overcomplicating. Let's try again.

Correct Mesh Equations:
  • Mesh 1 ( \( i_1 \) ):
  • Resistors: 10Ω (current \( i_1 \)), 2Ω (current \( i_1 - i_2 \)), 5Ω (current \( i_1 - i_3 \))
  • Voltage source: 6V (polarity + on left, - on right; so in the direction of \( i_1 \), we go from + to -, so voltage drop is -6V)
  • KVL: \( 10i_1 + 2(i_1 - i_2) + 5(i_1 - i_3) - 6 = 0 \)
  • Simplify: \( 10i_1 + 2i_1 - 2i_2 + 5i_1 - 5i_3 - 6 = 0 \) → \( 17i_1 - 2i_2 - 5i_3 = 6 \) ...(1)
  • Mesh 2 ( \( i_2 \) ):
  • Resistors: 2Ω (current \( i_2 - i_1 \)), 4Ω (current \( i_2 \)), 1Ω (current \( i_2 - i_3 \))
  • Voltage source: 8V (polarity + on top, - on bottom; so in the direction of \( i_2 \) (clockwise), we go from - to +, so voltage rise is +8V)
  • KVL: \( -2(i_2 - i_1) + 4i_2 + 1(i_2 - i_3) + 8 = 0 \)
  • Simplify: \( -2i_2 + 2i_1 + 4i_2 + i_2 - i_3 + 8 = 0 \) → \( 2i_1 + 3i_2 - i_3 = -8 \) ...(2)
  • Mesh 3 ( \( i_3 \) ):
  • Resistors: 5Ω (current \( i_3 - i_1 \)), 1Ω (current \( i_3 - i_2 \)), 5Ω? Wait, no, the 5Ω is in mesh 3? Wait, the right branch: 5Ω, 6V source? No, the 5Ω is in mesh 3, and the 1Ω is between mesh 2 and 3, 5Ω in mesh 3, and the 6V source? Wait, no, the 6V source is in mesh 1, 8V in mesh 2 and 3. Let's correct mesh 3:
  • Mesh 3: 5Ω (current \( i_3 - i_1 \)), 1Ω (current \( i_3 - i_2 \)), and the 8V source? No, the 8V source is in the vertical branch, with + on top, - on bottom. So in mesh 3 (clockwise), we go from - to + of the 8V source, so voltage rise is +8V? Wait, no, the 8V source is between mesh 2 and 3. Let's re-express:

Actually, the 8V source is in the branch common to mesh 2 and 3, with + on top, - on bottom. So for mesh 2 (clockwise), going through the 8V source, we go from - to + (rise), and for mesh 3 (clockwise), we go from + to - (drop). Let's redo mesh 3:

  • Mesh 3: 5Ω (current \( i_3 - i_1 \)), 1Ω (current \( i_3 - i_2 \)), and the 8V source (voltage drop is -8V, since we go from + to - in the direction of \( i_3 \))
  • KVL: \( -5(i_3 - i_1) - 1(i_3 - i_2) - 8 = 0 \)
  • Simplify: \( -5i_3 + 5i_1 - i_3 + i_2 - 8 = 0 \) → \( 5i_1 + i_2 - 6i_3 = 8 \) ...(3)

Now we have three equations:

  1. \( 17i_1 - 2i_2 - 5i_3 = 6 \)
  2. \( 2i_1 + 3i_2 - i_3 = -8 \)
  3. \( 5i_1 + i_2 - 6i_3 = 8 \)

Let's solve equations 2 and 3 first. From equation 2: \( i_3 = 2i_1 + 3i_2 + 8 \)

Substitute \( i_3 \) into equation 3:

\( 5i_1 + i_2 - 6(2i_1 + 3i_2 + 8) = 8 \)

\( 5i_1 + i_2 - 12i_1 - 18i_2 - 48 = 8 \)

\( -7i_1 - 17i_2 = 56 \) → \( 7i_1 + 17i_2 = -56 \) ...(4)

Substitute \( i_3 = 2i_1 + 3i_2 + 8 \) into equation 1:

\( 17i_1 - 2i_2 - 5(2i_1 + 3i_2 + 8) = 6 \)

\( 17i_1 - 2i_2 - 10i_1 - 15i_2 - 40 = 6 \)

\( 7i_1 - 17i_2 = 46 \) ...(5)

Now we have equations (4) and (5):

Equation (4): \( 7i_1 + 17i_2 = -56 \)

Equation (5): \( 7i_1 - 17i_2 = 46 \)

Add equations (4) and (5):

\( 14i_1 = -10 \) → \( i_1 = -\frac{10}{14} = -\frac{5}{7} \) A

Substitute \( i_1 = -\frac{5}{7} \) into equation (4):

\( 7(-\frac{5}{7}) + 17i_2 = -56 \)

\( -5 + 17i_2 = -56 \) → \( 17i_2 = -51 \) → \( i_2 = -3 \) A

Now find \( i_3 \) from \( i_3 = 2i_1 + 3i_2 + 8 \):

\( i_3 = 2(-\frac{5}{7}) + 3(-3) + 8 = -\frac{10}{7} - 9 + 8 = -\frac{10}{7} - 1 = -\frac{17}{7} \) A

Now, \( i = i_2 - i_3 \) (since \( i_2 \) flows down through 1Ω, \( i_3 \) flows up, so net current up is \( i_2 - i_3 \)):

\( i = (-3) - (-\frac{17}{7}) = -3 + \frac{17}{7} = \frac{-21 + 17}{7} = -\frac{4}{7} \) A? Wait, that can't be right. Maybe I messed up the direction of \( i \).

Wait, maybe \( i = i_3 - i_2 \). Let's check the direction: the current \( i \) is upward. \( i_2 \) is clockwise in mesh 2, so through the 1Ω resistor, \( i_2 \) flows downward (since mesh 2 is clockwise: left branch 4Ω (down), 2Ω (up), 1Ω (down)? Wait, no, mesh 2: 4Ω is on the left, 2Ω is top, 1Ω is bottom. So \( i_2 \) flows: left branch 4Ω (down), top branch 2Ω (right to left, i.e., left), bottom branch 1Ω (right to left, i.e., left). Wait, maybe the direction of \( i \) is \( i_3 - i_2 \). Let's re-express:

If \( i \) is upward, then \( i_3 \) (clockwise in mesh 3) flows: right branch 5Ω (up), bottom branch 1Ω (up), left branch 8V (down). Wait, no, this is getting confusing. Let's use the correct KVL.

Alternative approach: Let's define the meshes correctly.

  • Mesh 1 (Top, \( i_1 \), clockwise):
  • Components: 10Ω (current \( i_1 \)), 6V source ( + on left, - on right, so voltage drop is -6V in direction of \( i_1 \)), 5Ω (current \( i_1 - i_3 \)), and 2Ω (current \( i_1 - i_2 \))? No, the 2Ω is between mesh 1 and 2, 1Ω between mesh 2 and 3, 4Ω in mesh 2, 5Ω in mesh 3, 10Ω and 6V in mesh 1, 8V in mesh 2 and 3.

Wait, maybe a better way:

  • Mesh 1: 10Ω, 6V (polarity + left, - right), 5Ω, and the 2Ω? No, the 2Ω is connected to the node between mesh 1 and 2, 1Ω between mesh 2 and 3, 4Ω in mesh 2, 5Ω in mesh 3, 10Ω and 6V in mesh 1, 8V in the vertical branch (between mesh 2 and 3).

Let's use the standard mesh analysis:

  1. Assign mesh currents \( i_1 \) (top), \( i_2 \) (left bottom), \( i_3 \) (right bottom), all clockwise.
  1. Mesh 1 ( \( i_1 \) ):
  • Resistors: 10Ω ( \( i_1 \) ), 2Ω ( \( i_1 - i_2 \) ), 5Ω ( \( i_1 - i_3 \) )
  • Voltage source: 6V ( + to - in direction of \( i_1 \), so voltage drop: -6V )
  • KVL: \( 10i_1 + 2(i_1 - i_2) + 5(i_1 - i_3) - 6 = 0 \)
  • Simplify: \( 10i_1 + 2i_1 - 2i_2 + 5i_1 - 5i_3 = 6 \) → \( 17i_1 - 2i_2 - 5i_3 = 6 \) ...(1)
  1. Mesh 2 ( \( i_2 \) ):
  • Resistors: 2Ω ( \( i_2 - i_1 \) ), 4Ω ( \( i_2 \) ), 1Ω ( \( i_2 - i_3 \) )
  • Voltage source: 8V ( - to + in direction of \( i_2 \), so voltage rise: +8V )
  • KVL: \( -2(i_2 - i_1) + 4i_2 + 1(i_2 - i_3) + 8 = 0 \)
  • Simplify: \( -2i_2 + 2i_1 + 4i_2 + i_2 - i_3 = -8 \) → \( 2i_1 + 3i_2 - i_3 = -8 \) ...(2)
  1. Mesh 3 ( \( i_3 \) ):
  • Resistors: 5Ω ( \( i_3 - i_1 \) ), 1Ω ( \( i_3 - i_2 \) ), 5Ω? No, the 5Ω is in mesh 3? Wait, the right branch is 5Ω, and the 8V source? No, the 8V source is in the vertical branch. Let's correct mesh 3:
  • Mesh 3: 5Ω ( \( i_3 - i_1 \) ), 1Ω ( \( i_3 - i_2 \) ), and the 8V source ( + to - in direction of \( i_3 \), so voltage drop: -8V )
  • KVL: \( -5(i_3 - i_1) - 1(i_3 - i_2) - 8 = 0 \)
  • Simplify: \( -5i_3 + 5i_1 - i_3 + i_2 - 8 = 0 \) → \( 5i_1 + i_2 - 6i_3 = 8 \) ...(3)

Now we have:

  1. \( 17i_1 - 2i_2 - 5i_3 = 6 \)
  1. \( 2i_1 + 3i_2 - i_3 = -8 \)
  1. \( 5i_1 + i_2 - 6i_3 = 8 \)

Let's solve equation (2) for \( i_3 \): \( i_3 = 2i_1 + 3i_2 + 8 \)

Substitute \( i_3 \) into equation (3):