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Question: Potential of point O in the given figure is $\frac{630}{47}KV$. Find K....

Potential of point O in the given figure is 63047KV\frac{630}{47}KV. Find K.

Answer

20/7

Explanation

Solution

The problem asks us to find the value of K, given the potential of point O in the circuit diagram. The potential of point O is given as 63047KV\frac{630}{47}KV.

We will use Kirchhoff's Current Law (KCL) at node O. KCL states that the algebraic sum of currents entering a node (or leaving a node) is zero. Let VOV_O be the potential at point O.

Let's analyze the currents leaving node O:

  1. Current towards 50V source (I1I_1): This current flows through the 5Ω resistor. I1=VO505I_1 = \frac{V_O - 50}{5}

  2. Current towards 30V source (I2I_2): This current flows through the 3Ω resistor. I2=VO303I_2 = \frac{V_O - 30}{3}

  3. Current towards 40V source (I3I_3): This current flows through the 4Ω resistor. I3=VO404I_3 = \frac{V_O - 40}{4}

  4. Current towards the right side (I4I_4): This current flows from O through a 2Ω resistor to a node, let's call it A. The most reasonable interpretation of the right side of the circuit is that the 2Ω resistor and the 3A current source are in parallel between node A and node B, and then a 2Ω resistor connects node B to node D. Since node D is not connected to anything else and its potential is unknown, we assume it's a floating node. For a floating node, the current leaving it must be zero. So, the current flowing into node D, IBD=VBVD2=0I_{BD} = \frac{V_B - V_D}{2} = 0, which implies VB=VDV_B = V_D.

    Now, let's apply KCL at node B: The current from the 2Ω resistor between A and B is VAVB2\frac{V_A - V_B}{2}. The current from the 3A current source is 3A (flowing from A to B). So, VAVB2+3=IBD=0\frac{V_A - V_B}{2} + 3 = I_{BD} = 0. VAVB2=3\frac{V_A - V_B}{2} = -3 VAVB=6V_A - V_B = -6 VA=VB6V_A = V_B - 6

    Now, let's apply KCL at node A: Current entering A from O is I4=VOVA2I_4 = \frac{V_O - V_A}{2}. Current leaving A towards B through 2Ω resistor is VAVB2\frac{V_A - V_B}{2}. Current leaving A towards B through 3A source is 3A. So, VOVA2=VAVB2+3\frac{V_O - V_A}{2} = \frac{V_A - V_B}{2} + 3. Substitute VAVB2=3\frac{V_A - V_B}{2} = -3: VOVA2=3+3\frac{V_O - V_A}{2} = -3 + 3 VOVA2=0\frac{V_O - V_A}{2} = 0 VOVA=0    VA=VOV_O - V_A = 0 \implies V_A = V_O.

    Since VA=VOV_A = V_O, the current I4=VOVA2=VOVO2=0I_4 = \frac{V_O - V_A}{2} = \frac{V_O - V_O}{2} = 0. This means no current flows into the right side of the circuit from node O. This simplifies the problem significantly, as the right branch effectively contributes zero current to node O.

Now, apply KCL at node O, considering only the first three branches: I1+I2+I3=0I_1 + I_2 + I_3 = 0 VO505+VO303+VO404=0\frac{V_O - 50}{5} + \frac{V_O - 30}{3} + \frac{V_O - 40}{4} = 0

To eliminate denominators, multiply the entire equation by the least common multiple (LCM) of 5, 3, and 4, which is 60. 60(VO505)+60(VO303)+60(VO404)=060 \left( \frac{V_O - 50}{5} \right) + 60 \left( \frac{V_O - 30}{3} \right) + 60 \left( \frac{V_O - 40}{4} \right) = 0 12(VO50)+20(VO30)+15(VO40)=012(V_O - 50) + 20(V_O - 30) + 15(V_O - 40) = 0 12VO600+20VO600+15VO600=012V_O - 600 + 20V_O - 600 + 15V_O - 600 = 0 Combine terms with VOV_O: (12+20+15)VO(600+600+600)=0(12 + 20 + 15)V_O - (600 + 600 + 600) = 0 47VO1800=047V_O - 1800 = 0 47VO=180047V_O = 1800 VO=180047VV_O = \frac{1800}{47} V

The problem states that the potential of point O is 63047KV\frac{630}{47}KV. We calculated VO=180047VV_O = \frac{1800}{47} V. To compare, we need to convert units. 1KV=1000V1 KV = 1000 V. So, 63047KV=63047×1000V=63000047V\frac{630}{47} KV = \frac{630}{47} \times 1000 V = \frac{630000}{47} V.

This is a mismatch. Let's re-check the problem statement and the interpretation. Perhaps the "KV" in the problem statement was a typo and meant just "V". If so, K=1800/630K = 1800/630. K=1800630=18063=207K = \frac{1800}{630} = \frac{180}{63} = \frac{20}{7}. This is not an integer.

Let's assume the given potential 63047KV\frac{630}{47}KV is actually 63047×KV\frac{630}{47} \times K V. So, VO=63047KVV_O = \frac{630}{47} K V. We found VO=180047VV_O = \frac{1800}{47} V. Equating the two expressions for VOV_O: 63047K=180047\frac{630}{47} K = \frac{1800}{47} (assuming K is a dimensionless multiplier for the voltage in Volts, or if KV is meant as K * Volts) 630K=1800630 K = 1800 K=1800630=18063K = \frac{1800}{630} = \frac{180}{63} Divide by 9: K=207K = \frac{20}{7}. This is not an integer.

Let's re-read "Potential of point O in the given figure is 63047KV\frac{630}{47}KV". This means the value of potential is 63047\frac{630}{47} kiloVolts. It's not 63047×KV\frac{630}{47} \times K V. The question asks to "Find K". This implies K is a part of the numerical value given, not a unit. So, the given potential is VO=63047×1000V=63000047VV_O = \frac{630}{47} \times 1000 V = \frac{630000}{47} V.

Our calculated value is VO=180047VV_O = \frac{1800}{47} V. There seems to be a discrepancy between the calculated value and the given value. Let's re-verify the KCL equations and calculations. 12VO600+20VO600+15VO600=012V_O - 600 + 20V_O - 600 + 15V_O - 600 = 0 47VO1800=047V_O - 1800 = 0 47VO=180047V_O = 1800 VO=180047VV_O = \frac{1800}{47} V. The calculation is correct.

The only way for the problem to make sense is if the "KV" unit in the problem statement was meant to imply that the value KK is related to VOV_O such that VO=63047×KV_O = \frac{630}{47} \times K. And the final unit for VOV_O would be Volts. If VO=63047KV_O = \frac{630}{47} K Volts, then: 63047K=180047\frac{630}{47} K = \frac{1800}{47} 630K=1800630 K = 1800 K=1800630=18063=207K = \frac{1800}{630} = \frac{180}{63} = \frac{20}{7}. This is a rational number, but typically K is expected to be an integer in such problems.

Let's consider if the question meant the value of VOV_O is 63047×1000\frac{630}{47} \times 1000 and we need to find KK such that VO=KV_O = K. This would be trivial. Or if VO=K47VV_O = \frac{K}{47}V and KK is 630×1000630 \times 1000.

Let's assume the question means that the potential at point O is 63047\frac{630}{47} Volts, and we need to find the value of K such that VO=KV_O = K. This would mean K=63047K = \frac{630}{47}. But this is not how the question is phrased.

The most common interpretation of "Potential of point O in the given figure is 63047KV\frac{630}{47}KV. Find K." is that VO=63047×1000V_O = \frac{630}{47} \times 1000 Volts, and somewhere in the circuit, there's a parameter KK that needs to be found. But there is no parameter KK in the circuit diagram.

Given the phrasing "Potential of point O in the given figure is 63047KV\frac{630}{47}KV. Find K.", it implies that the value 63047\frac{630}{47} is given in a specific unit (KV), and we need to find a numerical factor 'K' that relates to this value. It's highly probable that the question intends for the numerical value of VOV_O to be K×63047K \times \frac{630}{47} Volts (or some other form), and we need to find KK.

Let's assume the given potential VO=63047×K0V_O = \frac{630}{47} \times K_0 Volts, where K0K_0 is 1000 if the unit is KV. And we need to find KK as a multiplier for the voltage. If the question is "Potential of point O is XX V. Find K.", and X=63047KX = \frac{630}{47} K. Then 63047K=180047\frac{630}{47} K = \frac{1800}{47}. K=1800630=18063=207K = \frac{1800}{630} = \frac{180}{63} = \frac{20}{7}.

If the question is "Potential of point O is KK V. Find K.", and K=63047×1000K = \frac{630}{47} \times 1000. This is not how it is written.

Let's consider that the given potential is VO=63047KV=63000047VV_O = \frac{630}{47} KV = \frac{630000}{47} V. And the question asks to find KK, where KK is a numerical factor in the answer. If the answer is KK, and the potential is 63047KV\frac{630}{47}KV, it implies the numerical value of VOV_O is KK times some base value. This is a poorly worded question if KK is not part of the circuit. However, in competitive exams, sometimes questions are phrased like "The value of X is 5Y. Find Y." where Y is the calculated value.

Let's assume the question implies that the calculated potential VOV_O is given as 63047KV\frac{630}{47}KV. So, V_O_{calculated} = \frac{1800}{47} V. And V_O_{given} = \frac{630}{47} KV = \frac{630}{47} \times 1000 V = \frac{630000}{47} V. These two values are not equal. This suggests either a typo in the question's given value or a misinterpretation of the circuit.

Let's re-examine the circuit for alternative interpretations of the right side. The interpretation of the right side (2Ω || 3A source) between A and B, and D being floating, leads to VA=VOV_A = V_O and I4=0I_4=0. This is a very strong result. If this is true, then the problem is simply KCL at O for the first three branches.

What if D is grounded? VD=0V_D = 0. Then from KCL at B: VAVB2+3=VB02\frac{V_A - V_B}{2} + 3 = \frac{V_B - 0}{2} VAVB+6=VBV_A - V_B + 6 = V_B VA+6=2VBV_A + 6 = 2V_B (Eq 1')

From KCL at A: VOVA2=VAVB2+3\frac{V_O - V_A}{2} = \frac{V_A - V_B}{2} + 3 VOVA=VAVB+6V_O - V_A = V_A - V_B + 6 VO+VB6=2VAV_O + V_B - 6 = 2V_A (Eq 2')

From (Eq 1'), VB=VA+62V_B = \frac{V_A+6}{2}. Substitute into (Eq 2'): VO+VA+626=2VAV_O + \frac{V_A+6}{2} - 6 = 2V_A 2VO+VA+612=4VA2V_O + V_A + 6 - 12 = 4V_A 2VO6=3VA2V_O - 6 = 3V_A VA=2VO63V_A = \frac{2V_O - 6}{3}

Now, substitute VAV_A into I4=VOVA2I_4 = \frac{V_O - V_A}{2}: I4=VO2VO632=3VO(2VO6)32=VO+66I_4 = \frac{V_O - \frac{2V_O - 6}{3}}{2} = \frac{\frac{3V_O - (2V_O - 6)}{3}}{2} = \frac{V_O + 6}{6}

Now, KCL at O: VO505+VO303+VO404+VO+66=0\frac{V_O - 50}{5} + \frac{V_O - 30}{3} + \frac{V_O - 40}{4} + \frac{V_O + 6}{6} = 0 Multiply by LCM of 5, 3, 4, 6 which is 60. 12(VO50)+20(VO30)+15(VO40)+10(VO+6)=012(V_O - 50) + 20(V_O - 30) + 15(V_O - 40) + 10(V_O + 6) = 0 12VO600+20VO600+15VO600+10VO+60=012V_O - 600 + 20V_O - 600 + 15V_O - 600 + 10V_O + 60 = 0 (12+20+15+10)VO(600+600+60060)=0(12 + 20 + 15 + 10)V_O - (600 + 600 + 600 - 60) = 0 57VO(180060)=057V_O - (1800 - 60) = 0 57VO=174057V_O = 1740 VO=174057V_O = \frac{1740}{57} 1740/57=30.526...1740/57 = 30.526... This is not 180047\frac{1800}{47}.

This confirms that the assumption of D being floating is the most likely intended scenario for a solvable problem with a "nice" fraction. The result VO=180047VV_O = \frac{1800}{47} V is robust under the assumption that D is floating and the current source is in parallel with the 2Ω resistor.

Given the problem statement "Potential of point O in the given figure is 63047KV\frac{630}{47}KV. Find K.", it is highly probable that the question intends for the numerical value of the potential (in Volts) to be K×63047K \times \frac{630}{47}. So, VO=63047KV_O = \frac{630}{47} K Volts. We calculated VO=180047V_O = \frac{1800}{47} Volts. Equating these two: 63047K=180047\frac{630}{47} K = \frac{1800}{47} 630K=1800630 K = 1800 K=1800630=18063K = \frac{1800}{630} = \frac{180}{63} Divide numerator and denominator by 9: K=207K = \frac{20}{7}

This is the most consistent interpretation given the numerical values. The "KV" unit in the problem statement might be a distractor or a poorly placed "K". If "KV" means kiloVolts, then the given potential is 63000047V\frac{630000}{47}V, which does not match our calculation.

Final check of the interpretation of the right side: If VA=VOV_A = V_O, then I4=0I_4 = 0. The KCL at A was (VOVA)/2=(VAVB)/2+3(V_O - V_A)/2 = (V_A - V_B)/2 + 3. If VA=VOV_A = V_O, then 0=(VOVB)/2+30 = (V_O - V_B)/2 + 3. (VOVB)/2=3(V_O - V_B)/2 = -3. VOVB=6V_O - V_B = -6. VB=VO+6V_B = V_O + 6. From KCL at B, (VAVB)/2+3=0(V_A - V_B)/2 + 3 = 0 (since VB=VDV_B = V_D implies current to D is 0). Substitute VA=VOV_A = V_O: (VOVB)/2+3=0(V_O - V_B)/2 + 3 = 0. This is consistent with the previous step. So, the interpretation that I4=0I_4 = 0 (and thus VA=VOV_A = V_O) is self-consistent under the assumption that D is a floating node.

The value of K is 207\frac{20}{7}.

The final answer is 207\boxed{\frac{20}{7}}.

Explanation of the solution:

  1. Identify node O and the branches connected to it.
  2. Apply Kirchhoff's Current Law (KCL) at node O: The sum of currents leaving node O is zero.
  3. For the rightmost branch, assume the 2Ω resistor and 3A current source are in parallel between two intermediate nodes, A and B. Node D is a floating node, meaning no current leaves it (ID=0I_D = 0).
  4. Apply KCL at node B: Current from (A to B) through 2Ω + Current from 3A source = Current to D. This leads to VAVB2+3=0\frac{V_A - V_B}{2} + 3 = 0, so VAVB=6V_A - V_B = -6.
  5. Apply KCL at node A: Current from (O to A) through 2Ω = Current from (A to B) through 2Ω + Current from 3A source. This leads to VOVA2=VAVB2+3\frac{V_O - V_A}{2} = \frac{V_A - V_B}{2} + 3.
  6. Substitute the result from KCL at B into KCL at A: VOVA2=3+3=0\frac{V_O - V_A}{2} = -3 + 3 = 0. This implies VOVA=0V_O - V_A = 0, so VA=VOV_A = V_O.
  7. Since VA=VOV_A = V_O, the current from O to A (I4I_4) is zero. This means the rightmost branch does not draw any current from node O.
  8. Simplify KCL at node O by considering only the first three branches: VO505+VO303+VO404=0\frac{V_O - 50}{5} + \frac{V_O - 30}{3} + \frac{V_O - 40}{4} = 0.
  9. Solve for VOV_O: Multiply by the LCM of 5, 3, 4 (which is 60) to clear denominators. 12(VO50)+20(VO30)+15(VO40)=012(V_O - 50) + 20(V_O - 30) + 15(V_O - 40) = 0 12VO600+20VO600+15VO600=012V_O - 600 + 20V_O - 600 + 15V_O - 600 = 0 47VO1800=047V_O - 1800 = 0 VO=180047VV_O = \frac{1800}{47} V.
  10. The problem states that the potential of point O is 63047KV\frac{630}{47}KV. Interpreting this as VO=63047KV_O = \frac{630}{47} K Volts, and equating it to the calculated value: 63047K=180047\frac{630}{47} K = \frac{1800}{47} 630K=1800630 K = 1800 K=1800630=18063=207K = \frac{1800}{630} = \frac{180}{63} = \frac{20}{7}.

Answer: The value of K is 207\frac{20}{7}.