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Question: How will you connect (series and parallel) 24 cells each of internal resistance 1 $\Omega$ to get ma...

How will you connect (series and parallel) 24 cells each of internal resistance 1 Ω\Omega to get maximum power output across a load of 10 Ω\Omega?

Answer

Connect 12 cells in series to form each row, and connect 2 such rows in parallel.

Explanation

Solution

For maximum power transfer, the total internal resistance of the battery combination (rtotalr_{total}) should be equal to the load resistance (RR). Let mm be the number of cells in series in each row, and nn be the number of parallel rows. The total number of cells is N=m×n=24N = m \times n = 24. The total internal resistance of the combination is rtotal=m×rnr_{total} = \frac{m \times r}{n}, where rr is the internal resistance of a single cell.

Given r=1Ωr = 1 \Omega and R=10ΩR = 10 \Omega. For maximum power transfer, rtotal=Rr_{total} = R, so m×1n=10\frac{m \times 1}{n} = 10, which means m=10nm = 10n.

We have two equations:

  1. m×n=24m \times n = 24
  2. m=10nm = 10n

Substituting (2) into (1): (10n)×n=24(10n) \times n = 24 10n2=2410n^2 = 24 n2=2.4n^2 = 2.4 n=2.4n = \sqrt{2.4}

Since mm and nn must be integers, we cannot achieve perfect matching. We need to find integer pairs (m,n)(m, n) such that m×n=24m \times n = 24 and mn\frac{m}{n} is closest to 1010.

Let's list possible integer pairs (m,n)(m, n) and their corresponding rtotal=mnr_{total} = \frac{m}{n}:

  • (m=1,n=24)    rtotal=1/240.04Ω(m=1, n=24) \implies r_{total} = 1/24 \approx 0.04 \Omega
  • (m=2,n=12)    rtotal=2/120.167Ω(m=2, n=12) \implies r_{total} = 2/12 \approx 0.167 \Omega
  • (m=3,n=8)    rtotal=3/8=0.375Ω(m=3, n=8) \implies r_{total} = 3/8 = 0.375 \Omega
  • (m=4,n=6)    rtotal=4/60.667Ω(m=4, n=6) \implies r_{total} = 4/6 \approx 0.667 \Omega
  • (m=6,n=4)    rtotal=6/4=1.5Ω(m=6, n=4) \implies r_{total} = 6/4 = 1.5 \Omega
  • (m=8,n=3)    rtotal=8/32.667Ω(m=8, n=3) \implies r_{total} = 8/3 \approx 2.667 \Omega
  • (m=12,n=2)    rtotal=12/2=6Ω(m=12, n=2) \implies r_{total} = 12/2 = 6 \Omega
  • (m=24,n=1)    rtotal=24/1=24Ω(m=24, n=1) \implies r_{total} = 24/1 = 24 \Omega

The ideal rtotalr_{total} is 10Ω10 \Omega. The closest values are 6Ω6 \Omega and 24Ω24 \Omega. The power delivered to the load is P=m2E2R(R+rtotal)2P = \frac{m^2 \mathcal{E}^2 R}{(R + r_{total})^2}, where E\mathcal{E} is the emf of a single cell. To maximize power, we need to maximize the term R(R+rtotal)2\frac{R}{(R + r_{total})^2} for a fixed mm and E\mathcal{E}. Alternatively, considering the total emf Etotal=mEE_{total} = m\mathcal{E} and total internal resistance rtotal=mrnr_{total} = \frac{mr}{n}, the power is P=Etotal2R(R+rtotal)2P = \frac{E_{total}^2 R}{(R + r_{total})^2}. The power delivered is also given by P=NrtotalE2R(R+rtotal)2P = \frac{N \cdot r_{total} \cdot \mathcal{E}^2 \cdot R}{(R + r_{total})^2} where N=24N=24. P=24rtotalE210(10+rtotal)2P = \frac{24 \cdot r_{total} \cdot \mathcal{E}^2 \cdot 10}{(10 + r_{total})^2}. We need to maximize f(rtotal)=rtotal(10+rtotal)2f(r_{total}) = \frac{r_{total}}{(10+r_{total})^2}. The derivative f(rtotal)=10rtotal(10+rtotal)3f'(r_{total}) = \frac{10-r_{total}}{(10+r_{total})^3}. Setting f(rtotal)=0f'(r_{total})=0 gives rtotal=10r_{total}=10.

Let's evaluate f(rtotal)f(r_{total}) for the closest values:

  • For rtotal=6Ωr_{total} = 6 \Omega (when m=12,n=2m=12, n=2): f(6)=6(10+6)2=6256f(6) = \frac{6}{(10+6)^2} = \frac{6}{256}.
  • For rtotal=24Ωr_{total} = 24 \Omega (when m=24,n=1m=24, n=1): f(24)=24(10+24)2=241156f(24) = \frac{24}{(10+24)^2} = \frac{24}{1156}.

Comparing the values: 62560.0234375\frac{6}{256} \approx 0.0234375 2411560.02076\frac{24}{1156} \approx 0.02076

Since 6256>241156\frac{6}{256} > \frac{24}{1156}, the power output is maximized when rtotal=6Ωr_{total} = 6 \Omega. This corresponds to the configuration where m=12m=12 (cells in series per row) and n=2n=2 (number of parallel rows). Therefore, connect 12 cells in series to form each row, and connect 2 such rows in parallel.