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STPM10 数据表(PDF) 39 Page - STMicroelectronics |
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STPM10 数据表(HTML) 39 Page - STMicroelectronics |
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39 / 51 page ![]() STPM10 Theory of operation Doc ID 17728 Rev 3 39/51 Equation 13 [see Figure 26 - 11] In this way, the AC part V•I•cos(2 ωt + ϕ)/2 has been removed from the instantaneous power. The absence of any AC component allows for a very fast calibration procedure. It requires only the setting of (using the internal device programming registers) the voltage and current sensor conversion constants, using the effective voltage and current (Vrms, Irms) readings provided by the device’s built-in communication port, avoiding the time-averaged readings of the active power or the need for line synchronization. 7.23.2 Reactive power The reactive power is produced using the previously-computed signals. In case of shunt sensor the voltage signal is derived while the current signal is not. A first computation is to multiply the DS value of the integrated voltage channel with the value of the integrated current channel, which yields: Equation 14 The second is to multiply the filtered DS value of the voltage channel with the value of the filtered current channel: Equation 15 From the above results, Q1(t) is proportional to 1/ ω, while Q2(t) is proportional to ω. The correct reactive power would result from the following formula: Equation 16 Since the above computation would need significant additional circuitry, the reactive power in the STPM10 is calculated using only the Q1(t) multiplied by ω, which means: Equation 17 2 cos I V 2 )) t ( p ) t ( p ( ) t ( p 1 2 ϕ ⋅ ⋅ = / − / = ()) t 2 sin( sin 2 VI t cos( I ) t sin V ( ) t ( I ) t ( v ) t ( I dt ) t ( v ) t ( Q1 ϕ + ω − ϕ ⋅ ω = ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ ϕ + ω ω − ⋅ ω = ⋅ = ⋅ ′ = ∫ ()) t 2 sin( sin 2 VI ) t sin( I t cos V ) t ( i ) t ( v ) t ( Q 2 ϕ + ω + ϕ ⋅ ω ⋅ = ϕ + ω ⋅ ω ω = ⋅ ′ = ϕ = ω ⋅ + ω ⋅ ⋅ = sin 2 VI 1 ) t ( Q ) t ( Q 2 1 Q 2 1 |
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