The noise power is given by the following formula (see https://en.wikipedia.org/wiki/Johnson–Nyquist_noise):
P = k B T Δ f P =k_BT\Delta f P = k B T Δ f where k B = 1.38 × 1 0 − 23 J / K k_B = 1.38\times 10^{-23}J/K k B = 1.38 × 1 0 − 23 J / K is the Boltzmann's constant, T = 37 ° C = 310 K T = 37\degree C = 310K T = 37° C = 310 K is the absolute temperature, and Δ f = 1 × 1 0 6 H z \Delta f = 1\times 10^{6}Hz Δ f = 1 × 1 0 6 Hz is the bandwidth. Thus, obtian:
P = 1.38 × 1 0 − 23 ⋅ 310 K ⋅ 1 0 6 = 4.28 × 1 0 − 15 W P = 1.38\times 10^{-23}\cdot 310K\cdot 10^{6} = 4.28\times 10^{-15}W P = 1.38 × 1 0 − 23 ⋅ 310 K ⋅ 1 0 6 = 4.28 × 1 0 − 15 W The noise voltage is:
E = 4 R k B T Δ f E = \sqrt{4Rk_BT\Delta f} E = 4 R k B T Δ f where R = 1 M Ω = 1 0 6 Ω R = 1M\Omega = 10^{6}\Omega R = 1 M Ω = 1 0 6 Ω is the resistance. Thus, obtain:
E = 4 ⋅ 1 0 6 ⋅ 1.38 × 1 0 − 23 ⋅ 310 ⋅ 1 0 6 ≈ 1.31 × 1 0 − 4 V E = \sqrt{4\cdot 10^6\cdot 1.38\times 10^{-23}\cdot 310\cdot 10^6} \approx 1.31\times 10^{-4}V E = 4 ⋅ 1 0 6 ⋅ 1.38 × 1 0 − 23 ⋅ 310 ⋅ 1 0 6 ≈ 1.31 × 1 0 − 4 V Answer. 4.28 × 1 0 − 15 W 4.28\times 10^{-15}W 4.28 × 1 0 − 15 W and 1.31 × 1 0 − 4 V 1.31\times 10^{-4}V 1.31 × 1 0 − 4 V .
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