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STPM01 数据表(PDF) 45 Page - STMicroelectronics |
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STPM01 数据表(HTML) 45 Page - STMicroelectronics |
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45 / 56 page ![]() STPM01 Theory of operation 45/56 DS value of integrated voltage channel with the value of integrated current channel, which yields: [Eq. 13] The second is to multiply filtered DS value of voltage channel with the value of filtered current channel, [Eq. 14] From the above results, Q1(t) is proportional to 1/ ωwhile Q2(t) is proportional to ω. The correct reactive power would result from the following formula: [Eq. 15] Since the above computation would need significant additional circuitry, the Reactive Power in the STPM01 is calculated using only the Q1(t) multiplied by ω, it means: [Eq. 16] The Reactive Power will present then a ripple at twice the line frequency. Since the average value of a sinusoid is 0, this ripple does not contribute to the reactive energy calculation over time, moreover, in the STPM01 the reactive power is not used for meter calibration or to generate the stepper pulses, then this ripple will not affect the overall system performances. In case of Rogowsky coil, the same procedure is applied, but the current channel will be proportional to the derived of the current and the differentiated is bypassed in the voltage channel, so we have: [Eq. 17] [Eq. 18] The reactive power is then calculated: [Eq. 19] ()) 2 sin( sin 2 cos( ) sin ( ) ( ) ( ) ( ) ( ) ( 1 ϕ ω ϕ ω ϕ ω ω ω + − ⋅ = ⎟ ⎠ ⎞ ⎜ ⎝ ⎛ + − ⋅ = ⋅ = ⋅ ′ = ∫ t VI t I t V t I t v t I dt t v t Q ()) 2 sin( sin 2 ) sin( cos ) ( ) ( ) ( 2 ϕ ω ϕ ω ϕ ω ω ω + + ⋅ ⋅ = + ⋅ = ⋅ ′ = t VI t I t V t i t v t Q ϕ ω ω sin 2 1 ) ( ) ( 2 1 2 1 VI t Q t Q Q = ⋅ + ⋅ ⋅ = ()) 2 sin( sin 2 ) ( 2 1 ) ( 1 3 ϕ ω ϕ ω + − ⋅ = ⋅ ⋅ = t VI t Q t Q () ()) 2 sin( sin 2 ) sin( ) cos( ) ( ) ( ) ( ) ( ) ( 1 ϕ ω ϕ ω ϕ ω ω ω + + = + − ⋅ ⎟ ⎠ ⎞ ⎜ ⎝ ⎛− = ⋅ = ′ ⋅ = ∫∫ t VI t I t V t i t V dt t i dt t v t Q () ()) 2 sin( sin 2 ) cos( ) ( sin ) ( ) ( ) ( 1 ϕ ω ϕ ω ϕ ω ω ω + − ⋅ ⋅ − = + − ⋅ = ′ ⋅ = t VI t I t t V t i t v t Q ()) 2 sin( sin 2 ) ( 2 1 ) ( 1 3 ϕ ω ϕ ω + + ⋅ = ⋅ ⋅ = t VI t Q t Q |
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