{"id":16675,"date":"2026-11-02T20:03:30","date_gmt":"2026-11-03T00:03:30","guid":{"rendered":"https:\/\/zobi.alcowep.com\/bourtagshdrevxnls658739\/tb-26-09-measured-hammer-tap-inputs\/"},"modified":"2026-11-02T20:03:30","modified_gmt":"2026-11-03T00:03:30","slug":"tb-26-09-measured-hammer-tap-inputs","status":"publish","type":"post","link":"https:\/\/zobi.alcowep.com\/bourtagshdrevxnls658739\/tb-26-09-measured-hammer-tap-inputs\/","title":{"rendered":"TB 26-09 Measured Hammer-Tap Inputs"},"content":{"rendered":"<h2 style=\"text-align: center\">TB 26-09 Measured Hammer-Tap Inputs<\/h2>\n<p><!-- no image --><\/p>\n<p class=\"wp-block-paragraph\"><em>For more information, contact Joel W. Sills, Langley Research Center, <\/em><a href=\"mailto:joel.w.sills@nasa.gov\">joel.w.sills@nasa.gov<\/a>.<\/p>\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09.pdf?emrc=d74e4e\">Download the PDF version<\/a><\/p>\n<p class=\"wp-block-paragraph\">An instrumented hammer test does not require an idealized single half-sine waveform. When the complete force and response are measured accurately, crest ripples and separated contacts remain known inputs. Force shape changes excitation, but does not inherently invalidate the record. Adequacy depends on measurement accuracy, bandwidth, signal-to-noise ratio, and coverage of the test objective. <\/p>\n<div class=\"hds-media hds-module wp-block-image\">\n<div class=\"margin-left-auto margin-right-auto nasa-block-align-inline\">\n<div class=\"hds-media-wrapper margin-left-auto margin-right-auto\">\n<figure class=\"hds-media-inner hds-cover-wrapper hds-media-ratio-fit \"><a href=\"https:\/\/www.nasa.gov\/wp-content\/uploads\/2015\/04\/tb-26-09-1-illustrative-hammer-force-time-histories.png\"><img decoding=\"async\" width=\"1366\" height=\"1074\" src=\"https:\/\/www.nasa.gov\/wp-content\/uploads\/2015\/04\/tb-26-09-1-illustrative-hammer-force-time-histories.png?w=1366\" class=\"attachment-2048x2048 size-2048x2048\" alt=\"\" loading=\"lazy\" srcset=\"https:\/\/www.nasa.gov\/wp-content\/uploads\/2015\/04\/tb-26-09-1-illustrative-hammer-force-time-histories.png 1366w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2015\/04\/tb-26-09-1-illustrative-hammer-force-time-histories.png?resize=300,236 300w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2015\/04\/tb-26-09-1-illustrative-hammer-force-time-histories.png?resize=768,604 768w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2015\/04\/tb-26-09-1-illustrative-hammer-force-time-histories.png?resize=1024,805 1024w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2015\/04\/tb-26-09-1-illustrative-hammer-force-time-histories.png?resize=400,314 400w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2015\/04\/tb-26-09-1-illustrative-hammer-force-time-histories.png?resize=600,472 600w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2015\/04\/tb-26-09-1-illustrative-hammer-force-time-histories.png?resize=900,708 900w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2015\/04\/tb-26-09-1-illustrative-hammer-force-time-histories.png?resize=1200,943 1200w\" sizes=\"auto, (max-width: 1366px) 100vw, 1366px\"><\/a><\/figure>\n<\/div>\n<\/div>\n<\/div>\n<p class=\"wp-block-paragraph\"><strong>Background: What the Hammer Actually Measures <\/strong><br \/>Hammer tests support modal analysis [2\u20134] and can precede pyroshock testing [6]. Figure 1 compares a half-sine, maintained-contact rippling, and separated contacts. During a zero-force interval, the structure continues to vibrate; re-contact acts on that vibration.<br \/><img loading=\"lazy\" decoding=\"async\" width=\"1308\" height=\"134\" class=\"wp-image-1061307\" src=\"https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-20-09-equation-.png\" alt=\"\" srcset=\"https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-20-09-equation-.png 1308w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-20-09-equation-.png?resize=300,31 300w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-20-09-equation-.png?resize=768,79 768w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-20-09-equation-.png?resize=1024,105 1024w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-20-09-equation-.png?resize=400,41 400w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-20-09-equation-.png?resize=600,61 600w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-20-09-equation-.png?resize=900,92 900w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-20-09-equation-.png?resize=1200,123 1200w\" sizes=\"auto, (max-width: 1308px) 100vw, 1308px\"><\/p>\n<p class=\"wp-block-paragraph\">If an exact model and test article receive the same force and initial conditions, uniqueness gives identical responses for each bounded measured history. An approximate model can show different errors as inputs excite different frequencies, amplitudes, or nonlinear states. See [1] for the exact-model derivation.<\/p>\n<div class=\"hds-media hds-module wp-block-image\">\n<div class=\"margin-left-auto margin-right-auto nasa-block-align-inline\">\n<div class=\"hds-media-wrapper margin-left-auto margin-right-auto\">\n<figure class=\"hds-media-inner hds-cover-wrapper hds-media-ratio-fit \"><a href=\"https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09-3-sepctra-of-figure-1-.png\"><img decoding=\"async\" width=\"1346\" height=\"798\" src=\"https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09-3-sepctra-of-figure-1-.png?w=1346\" class=\"attachment-2048x2048 size-2048x2048\" alt=\"\" loading=\"lazy\" srcset=\"https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09-3-sepctra-of-figure-1-.png 1346w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09-3-sepctra-of-figure-1-.png?resize=300,178 300w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09-3-sepctra-of-figure-1-.png?resize=768,455 768w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09-3-sepctra-of-figure-1-.png?resize=1024,607 1024w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09-3-sepctra-of-figure-1-.png?resize=400,237 400w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09-3-sepctra-of-figure-1-.png?resize=600,356 600w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09-3-sepctra-of-figure-1-.png?resize=900,534 900w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09-3-sepctra-of-figure-1-.png?resize=1200,711 1200w\" sizes=\"auto, (max-width: 1346px) 100vw, 1346px\"><\/a><\/figure>\n<\/div>\n<\/div>\n<\/div>\n<p class=\"wp-block-paragraph\"><strong>Analysis: A Half-Sine Is Broadband, but Not Flat<\/strong> <br \/>Figure 2 shows that a finite half-sine is broadband but contains spectral zeros at f\/fo = 3, 5, 7, \u2026, with fo = 1\/(2T) for pulse duration T. Its appearance alone cannot establish adequate excitation.<\/p>\n<p class=\"wp-block-paragraph\"><strong>Analysis: Spectral Content Is Determined by the Measured Force History<\/strong><br \/> Figure 3 normalizes each spectrum to its own DC value. Crest rippling adds content and can fill half-sine notches. Timing between separated contacts creates deterministic interference. For adequacy, inspect the unnormalized measured spectrum and response signal-to-noise ratio.<\/p>\n<div class=\"hds-media hds-module wp-block-image\">\n<div class=\"margin-left-auto margin-right-auto nasa-block-align-inline\">\n<div class=\"hds-media-wrapper margin-left-auto margin-right-auto\">\n<figure class=\"hds-media-inner hds-cover-wrapper hds-media-ratio-fit \"><a href=\"https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09-2-fourier-magnitude-normalized-to-dc.png\"><img decoding=\"async\" width=\"1356\" height=\"936\" src=\"https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09-2-fourier-magnitude-normalized-to-dc.png?w=1356\" class=\"attachment-2048x2048 size-2048x2048\" alt=\"\" loading=\"lazy\" srcset=\"https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09-2-fourier-magnitude-normalized-to-dc.png 1356w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09-2-fourier-magnitude-normalized-to-dc.png?resize=300,207 300w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09-2-fourier-magnitude-normalized-to-dc.png?resize=768,530 768w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09-2-fourier-magnitude-normalized-to-dc.png?resize=1024,707 1024w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09-2-fourier-magnitude-normalized-to-dc.png?resize=400,276 400w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09-2-fourier-magnitude-normalized-to-dc.png?resize=600,414 600w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09-2-fourier-magnitude-normalized-to-dc.png?resize=900,621 900w, https:\/\/www.nasa.gov\/wp-content\/uploads\/2026\/11\/tb-26-09-2-fourier-magnitude-normalized-to-dc.png?resize=1200,828 1200w\" sizes=\"auto, (max-width: 1356px) 100vw, 1356px\"><\/a><\/figure>\n<\/div>\n<\/div>\n<\/div>\n<p class=\"wp-block-paragraph\"><strong>Recommended Practice: Evaluate Test Adequacy Against the Intended Objective<\/strong><br \/>\u2022 Measure the complete applied force with adequate bandwidth, calibration, dynamic range, and time synchronization.<br \/>\u00a0\u2022 Verify that the response measurements have adequate bandwidth and signal-to-noise ratio and are not clipped or saturated.<br \/>\u00a0\u2022 Confirm that the excitation covers the frequency, amplitude, and nonlinear-response ranges required by the intended test objective.<br \/>\u2022 Reject or repeat a test only for an identified measurement, excitation, or coverage deficiency.<\/p>\n<p class=\"wp-block-paragraph\"><strong>Conclusion<\/strong><br \/> Half-sine appearance neither establishes validity nor guarantees adequacy. Judge each hammer test by its purpose and by accurate, complete force and response measurements over the required range.<\/p>\n<p class=\"wp-block-paragraph\"><strong>References<\/strong><br \/>1. A. Majed, J. Sills, E. Henkel, V. Babuska, S. Yunis, D. Hamilton, J. Akers, and T. Kinney, Validity and Predictability of Measured Hammer Tap Inputs: Linear and Nonlinear Structural Systems, September 2026.<br \/>2. D. J. Ewins, Modal Testing: Theory, Practice and Application, 2nd ed., 2000.<br \/>3. ISO 7626-5:2019, Mechanical Vibration and Shock\u2014Experimental Determination of Mechanical Mobility\u2014Part 5<br \/>4. K. G. McConnell and P. S. Varoto, Vibration Testing: Theory and Practice, 2nd ed., 2008.<br \/>5. A. H. Nayfeh and D. T. Mook, Nonlinear Oscillations, 1979. 6. NASA-STD-7003, Pyroshock Test Criteria, 1999<\/p>\n<p class=\"wp-block-paragraph\">\n<p class=\"wpematico_credit\"><small>Powered by <a href=\"http:\/\/www.wpematico.com\" target=\"_blank\">WPeMatico<\/a><\/small><\/p>\n<p><a href=\"https:\/\/www.nasa.gov\/centers-and-facilities\/nesc\/tb-26-09-measured-hammer-tap-inputs\/\" target=\"_blank\" rel=\"noopener\">Get The Details&#8230;<\/a><br \/>\nMeagan Chappell  <\/p>\n","protected":false},"excerpt":{"rendered":"<p>For more information, contact Joel W. Sills, Langley Research Center, joel.w.sills@nasa.gov. Download the PDF version An instrumented hammer test does not require an idealized single half-sine waveform. When the complete force and response are measured accurately, crest ripples and separated contacts remain known inputs. Force shape changes excitation, but does not inherently invalidate the record. 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