Question 18.QE.4: Hand-powered computer To power computers in locations not re......

Hand-powered computer

To power computers in locations not reached by any power grid, engineers have developed hand cranks that rotate a 100-turn coil in a strong magnetic field. In a quarter-turn of the crank of one of these devices, the magnetic flux through the coil’s area changes from 0 to 0.10 T ⋅ m² in 0.50 s. What is the average magnitude of the emf induced in the coil during this quarter-turn?

Represent mathematically    Faraday’s law [Eq. (18.3)] can be used to determine the average magnitude of the emf produced in the coil:

\varepsilon_{\text {in }}=N\left|\frac{\Delta \Phi}{\Delta t}\right|=N\left|\frac{\Delta[B A \cos \theta]}{\Delta t}\right|     (18.3)

\varepsilon_{\mathrm{in}}=N\left|\frac{\Delta \Phi}{\Delta t}\right|=N\left|\frac{\Phi_{\mathrm{f}}-\Phi_{\mathrm{i}}}{t_{\mathrm{f}}-t_{\mathrm{i}}}\right|

Step-by-Step
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Solve and evaluate    Inserting the appropriate values, we find:

\varepsilon_{\mathrm{in}}=(100)\left|\frac{\left(0.10 \mathrm{~T} \cdot \mathrm{m}^2\right)-0}{0.50 \mathrm{~s}-0}\right|=20 \mathrm{~V}

The magnitude of this emf is about what is required by laptop computers. However, the computer only works while the coil is turning. Laptops typically have a power requirement of about 50 watts (50 joules each second), which means considerable strength and  endurance would be needed to keep the coil rotating.

Try it yourself:    Determine the average emf produced in the coil if you turn the coil one quarter-turn in 1.0 s instead of in 0.50 s.

Answer:    10 V.

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