هذه
مقالة غير مراجعة .
ينبغي أن يزال هذا القالب بعد أن يراجعها محرر مغاير للذي أنشأها؛ إذا لزم الأمر فيجب أن توسم المقالة بقوالب الصيانة المناسبة. يمكن أيضاً تقديم طلب لمراجعة المقالة في الصفحة المخصصة لذلك. (يناير 2019 )
رسم بياني يوضح تشكيل الطور[(φ (t] وهي دالة غير خطية تتزايد من 0 إلى π / 2 خلال الفترة (t) ما بين 0 و 16 . ويعرف المكونان المؤلفان من تشكيل السعة باسم مكون متوافق الطور (I ، الخط الرفيع الأزرق، دالة تناقصية) ومكون تربيعي أو عامودي (Q ،الخط الرفيع الأحمر، دالة تزيادية).
في الهندسة الكهربائية ، يمكن تفكيك أو توليف الدالة الجيبية [ sin ( x ) ] ذات تشكيل زاوي (angle modulation ) من دالتين جيبية مشكّلة بالسعة (amplitude-modulated ) التي يتم تعويضها في الطور بربع دورة (π / 2 راديان). جميع الدوال الثلاث لها نفس التردد. تعرف الدوال الجيبية المشكلة بالسعة بالموجات العامودية متوافقة الطور. في بعض السياقات يكون من الملائم أكثر الإشارة إلى تشكيل السعة (القاعدي) فقط بهذه الشروط.[1]
عندما يتم تطبيق جهد جيبي إما على مكثف بسيط أو ملف كهربائي ، فإن التيار الناتج الذي يتدفق يتعامد "عامودي" مع الجهد.
نموذج الإشارة ذات النطاق الضيق
في تطبيقات تشكيل الزاوية، مع تردد الموجة الحاملة f, φ هي أيضاً دالة متغير الزمن،[2] :
*يحتاج تعديل هذا القسم*
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature . [3]
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mo stretchy="false">
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mn>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mn><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mo>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mo stretchy="false">
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mo stretchy="false">
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mo stretchy="false">
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mo>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mo>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mo stretchy="false">
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mn>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mn><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
mi><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mo stretchy="false">
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mo>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mo>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mo stretchy="false">
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mo stretchy="false">
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mo stretchy="false">
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mo stretchy="false">
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo></mrow><mo>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo></munder></mrow><mrow class="MJX-TeXAtom-ORD"><mtext>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mtext></mrow></munder><mo>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mo>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mrow><mo>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mrow><mn>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mn><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mo>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mrow class="MJX-TeXAtom-ORD"><mfrac><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mn>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mn></mfrac></mrow></mrow><mo>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo></mrow></mrow><mo>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo></mover></mrow><mrow class="MJX-TeXAtom-ORD"><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mo>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mo stretchy="false">
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mn>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mn><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mo stretchy="false">
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo></mrow></mover><mo>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mo>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mo stretchy="false">
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mo stretchy="false">
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mi>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mi><mo stretchy="false">
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo><mo stretchy="false">
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo></mrow><mo>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo></munder></mrow><mrow class="MJX-TeXAtom-ORD"><mtext>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mtext></mrow></munder><mo>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
</mo></mrow>
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature .
sin [ 2 π f t + ϕ ( t ) ] = sin ( 2 π f t ) ⋅ cos [ ϕ ( t ) ] ⏟ in-phase + sin ( 2 π f t + π 2 ) ⏞ cos ( 2 π f t ) ⋅ sin [ ϕ ( t ) ] ⏟ quadrature . [4]
</img>
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