An investigation of the constant-temperature hot-wire anemometer
An algorithm is developed for deriving the transfer functions of the constant-temperature hot-wire anemometer of arbitrary complexity. The only restriction is that the bridge elements, including the hot-wire filament, must be modeled by lumped components. A minimum of two equivalent amplifiers are r...
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Veröffentlicht in: | Experimental thermal and fluid science 1995-08, Vol.11 (2), p.117-134 |
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description | An algorithm is developed for deriving the transfer functions of the constant-temperature hot-wire anemometer of arbitrary complexity. The only restriction is that the bridge elements, including the hot-wire filament, must be modeled by lumped components. A minimum of two equivalent amplifiers are required to model the feedback amplifier properly. The poles of the transfer functions for electronic and velocity perturbations are shown to be identical regardless of the frequency response characteristics of the feedback amplifier and the nature and quantity of components used to model the bridge impedances. Computer simulations are used to explore the behavior of representative configurations. It is shown that the frequency response characteristics of the feedback amplifier must be included in addition to the offset voltage and cable and balance inductance to fully account for the behaviour observed in real systems. This leads to an optimum system response when the balance inductor is in excess of that required for ac bridge balance. Increasing the frequency response and gain of the feedback amplifier have the rather surprising effect of increasing the damping of the dominant poles. It is the higher order poles that are responsible for the instabilities under these conditions. With subminiature wires it is shown that insufficient frequency response of the feedback amplifier is the most likely cause of instabilities. Operating modes are demonstrated that are misleading, in the sense that the operator can be deceived into interpreting an erroneous frequency response. Examples are provided to help operators of the instrument to identify and avoid these rather subtle and undesirable modes of operation. A brief description is given of a new high-performance anemometer design that is based on these considerations. |
doi_str_mv | 10.1016/0894-1777(94)00137-W |
format | Article |
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The only restriction is that the bridge elements, including the hot-wire filament, must be modeled by lumped components. A minimum of two equivalent amplifiers are required to model the feedback amplifier properly. The poles of the transfer functions for electronic and velocity perturbations are shown to be identical regardless of the frequency response characteristics of the feedback amplifier and the nature and quantity of components used to model the bridge impedances. Computer simulations are used to explore the behavior of representative configurations. It is shown that the frequency response characteristics of the feedback amplifier must be included in addition to the offset voltage and cable and balance inductance to fully account for the behaviour observed in real systems. This leads to an optimum system response when the balance inductor is in excess of that required for ac bridge balance. Increasing the frequency response and gain of the feedback amplifier have the rather surprising effect of increasing the damping of the dominant poles. It is the higher order poles that are responsible for the instabilities under these conditions. With subminiature wires it is shown that insufficient frequency response of the feedback amplifier is the most likely cause of instabilities. Operating modes are demonstrated that are misleading, in the sense that the operator can be deceived into interpreting an erroneous frequency response. Examples are provided to help operators of the instrument to identify and avoid these rather subtle and undesirable modes of operation. 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Increasing the frequency response and gain of the feedback amplifier have the rather surprising effect of increasing the damping of the dominant poles. It is the higher order poles that are responsible for the instabilities under these conditions. With subminiature wires it is shown that insufficient frequency response of the feedback amplifier is the most likely cause of instabilities. Operating modes are demonstrated that are misleading, in the sense that the operator can be deceived into interpreting an erroneous frequency response. Examples are provided to help operators of the instrument to identify and avoid these rather subtle and undesirable modes of operation. A brief description is given of a new high-performance anemometer design that is based on these considerations.</description><subject>anemometer</subject><subject>Exact sciences and technology</subject><subject>Fluid dynamics</subject><subject>frequency response</subject><subject>Fundamental areas of phenomenology (including applications)</subject><subject>hot-wire</subject><subject>instability</subject><subject>Instrumentation for fluid dynamics</subject><subject>Physics</subject><subject>transfer function</subject><issn>0894-1777</issn><issn>1879-2286</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1995</creationdate><recordtype>article</recordtype><recordid>eNp9kE1LAzEURYMoWKv_wMUsRHQRzcdMMrMRS_ELCm6ULkPIvLGRmaQmacV_b2pLl65eIOfd3ByEzim5oYSKW1I3JaZSyqumvCaEconnB2hEa9lgxmpxiEZ75BidxPhJCKkZJSN0P3GFdWuIyX7oZL0rfFekBRTGu5i0SzjBsISg0ypAsfAJf9t80A4GP0CCcIqOOt1HONvNMXp_fHibPuPZ69PLdDLDphQiYdmWVdOYjlPBuOScUiYawQipNAVgUjaadNq0muUbwgwjEtqKGmi5oUR2fIwut7nL4L9Wua8abDTQ97mKX0XFZClkDs5guQVN8DEG6NQy2EGHH0WJ2uhSGxdq40Ll-adLzfPaxS5fR6P7LmhnbNzvckGritOM3W0xyH9dWwgqGgsu98xaTFKtt_-_8wv8UH3C</recordid><startdate>19950801</startdate><enddate>19950801</enddate><creator>Watmuff, Jonathan H.</creator><general>Elsevier Inc</general><general>Elsevier Science</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>19950801</creationdate><title>An investigation of the constant-temperature hot-wire anemometer</title><author>Watmuff, Jonathan H.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c466t-7d4599cf316237331126962005a1ee2779a0facda211202c207ed51ced3c107f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1995</creationdate><topic>anemometer</topic><topic>Exact sciences and technology</topic><topic>Fluid dynamics</topic><topic>frequency response</topic><topic>Fundamental areas of phenomenology (including applications)</topic><topic>hot-wire</topic><topic>instability</topic><topic>Instrumentation for fluid dynamics</topic><topic>Physics</topic><topic>transfer function</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Watmuff, Jonathan H.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Experimental thermal and fluid science</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Watmuff, Jonathan H.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>An investigation of the constant-temperature hot-wire anemometer</atitle><jtitle>Experimental thermal and fluid science</jtitle><date>1995-08-01</date><risdate>1995</risdate><volume>11</volume><issue>2</issue><spage>117</spage><epage>134</epage><pages>117-134</pages><issn>0894-1777</issn><eissn>1879-2286</eissn><abstract>An algorithm is developed for deriving the transfer functions of the constant-temperature hot-wire anemometer of arbitrary complexity. The only restriction is that the bridge elements, including the hot-wire filament, must be modeled by lumped components. A minimum of two equivalent amplifiers are required to model the feedback amplifier properly. The poles of the transfer functions for electronic and velocity perturbations are shown to be identical regardless of the frequency response characteristics of the feedback amplifier and the nature and quantity of components used to model the bridge impedances. Computer simulations are used to explore the behavior of representative configurations. It is shown that the frequency response characteristics of the feedback amplifier must be included in addition to the offset voltage and cable and balance inductance to fully account for the behaviour observed in real systems. This leads to an optimum system response when the balance inductor is in excess of that required for ac bridge balance. Increasing the frequency response and gain of the feedback amplifier have the rather surprising effect of increasing the damping of the dominant poles. It is the higher order poles that are responsible for the instabilities under these conditions. With subminiature wires it is shown that insufficient frequency response of the feedback amplifier is the most likely cause of instabilities. Operating modes are demonstrated that are misleading, in the sense that the operator can be deceived into interpreting an erroneous frequency response. Examples are provided to help operators of the instrument to identify and avoid these rather subtle and undesirable modes of operation. A brief description is given of a new high-performance anemometer design that is based on these considerations.</abstract><cop>New York, NY</cop><pub>Elsevier Inc</pub><doi>10.1016/0894-1777(94)00137-W</doi><tpages>18</tpages></addata></record> |
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source | ScienceDirect Journals (5 years ago - present) |
subjects | anemometer Exact sciences and technology Fluid dynamics frequency response Fundamental areas of phenomenology (including applications) hot-wire instability Instrumentation for fluid dynamics Physics transfer function |
title | An investigation of the constant-temperature hot-wire anemometer |
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