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STPM11ATR 数据表(PDF) 35 Page - STMicroelectronics |
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STPM11ATR 数据表(HTML) 35 Page - STMicroelectronics |
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35 / 46 page ![]() STPM11, STPM12, STPM13, STPM14 Energy calculation algorithm Doc ID 13167 Rev 8 35/46 In the STPM1x, after the pre-conditioning and the A/D conversion, the digital voltage signal (which is dynamically more stable with respect to the current signal) is processed by a differentiate stage which transforms: Equation 9 v(t) → v’(t) = dv/dt = V ⋅ ω ⋅ cos tω; (see [5] in Figure 22); The result, together with the pre-processed and digitalized current signal: Equation 10 i(t) = I ⋅ sin (tω + ϕ); (see [6] in Figure 22) can then be used to calculate. These digital signals are also used in two additional steps for integration, obtaining: Equation 11 dv/dt → v(t) = V ⋅ sin tω; (see [7] in Figure 22) Equation 12 (see [8] in Figure 22) Now four signals are available. Combining (pairing) them by two multiplication steps two results are obtained: Equation 13 (see [9] in Figure 22) Equation 14 (see [10] in Figure 22) After these two operations, another stage another step involves the subtraction of p1 from p2 and dividing the result by 2, to obtain the active power: Equation 15 (see [12] in Figure 22) In this way, the AC part ) t cos( I dt ) t ( i ) t ( I ϕ + ω ⋅ ω − = ⋅ = ∫ i(t) ⋅ 2 ) t 2 cos( I V 2 cos I V dt ) t ( i dt dv ) t ( p 1 ϕ + ω ⋅ ⋅ − ϕ ⋅ ⋅ − = ⋅ ⋅ = / ∫ 2 ) t 2 cos( I V 2 cos I V ) t ( i ) t ( v ) t ( p 2 ϕ + ω ⋅ ⋅ − ϕ ⋅ ⋅ = ⋅ = / 2 cos I V 2 )) t ( p ) t ( p ( ) t ( p 1 2 ϕ ⋅ ⋅ = / − / = Obsolete Product(s) - Obsolete Product(s) |
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