![](data:image/png;base64,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)
(3)
Индекс направленности Q – коэффициент направленности, выраженный в децибелах:
![](data:image/png;base64,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)
(4)
Ширина диаграммы направленности
![](data:image/png;base64,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)
определяется углом, в пределах которого чувствительность микрофона уменьшается не более чем в
![](data:image/png;base64,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)
раз относительно осевой чувствительности.
Перепад чувствительности «фронт-тыл» - отношение чувствительности микрофона при θ = 00 к чувствительности при θ = 1800.
В таблице 1 прведены значения этих характеристик направленности комбинированного микрофона для ряда значений параметра q.
Таблица 1. Характеристики комбинированных приёмников при разных значениях параметра q.
Управление диаграммой направленности может быть осуществлено, например, при включении микрофонов по схеме, изображенной на рис. 7.
![](data:image/png;base64,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)
Рисунок 7.
При верхнем положении движков потенциометров работает только приёмник давления (q = 0), микрофон – ненаправленный. При нижнем положении движков работает только приёмник градиента давления (q = 1), диаграмма направленности – косинусоидная. В промежуточных положениях движков получаются диаграммы направленности других видов (см. таблицу 6).
В некоторых случаях приёмник должен иметь более острую диаграмму направленности, чем у приёмников, рассмотренных выше. Такая задача может быть решена путем объединения нескольких одинаковых приёмников в группу.
Микрофоны располагают вдоль прямой линии на расстоянии d друг от друга, Выходы микрофонов соединяют последовательно (см. рис. 8).
![](data:image/png;base64,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)
Рисунок 8
Найдем характеристику направленности микрофона
.Будем считать, что плоская звуковая волна падает под углом θ к оси системы. Тогда между напряжениями соседних микрофонов будет иметь место сдвиг по фазе ![](data:image/png;base64,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)
где
, а напряжение i – го микрофона
. Суммируя напряжения всех микрофонов, получим:
.Амплитуда этого напряжения:
.При
это выражение даёт неопределенность вида 0/0. Раскрывая неопределенность по правилу Лопиталя, получим
. Тогда характеристика направленности:
(5)где
- характеристика направленности одного микрофона. Из выражения (5) следует, что диаграмма направленности может иметь несколько лепестков. Направления , для которых характеристика направленности принимает нулевые значения, можно определить из условия: ![](data:image/png;base64,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)
где
- целое число.Или иначе:
.Откуда число нулей диаграммы направленности
, т.е. чем больше размер линейки микрофонов, тем больше число лепестков диаграммы направленности и каждый лепесток становится уже. На рис. 9 приведены диаграммы направленности линейки из ненаправленных микрофонов для ряда частот. 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Диаграммы направленности линейки из 5 ненаправленных микрофонов.
. Кривая 1 для частоты 100 Гц, кривая 2 – для частоты 500 Гц, кривая 3 – для 1000 Гц.