US3918294A
Expired / Lapsed
US
⏱️ 0.0 years remaining
Axial force measuring method utilizing ultrasonic wave
Assignee: Toyota Motor Corp
•
Filing: 1974-03-29
•
Granted: 1975-11-11
•
Expires: 1994-03-29
Abstract
Abstract A method of measuring axial force existing in a bolt or the like from two natural resonant frequency values of the bolt, the one of which being obtained when the axial force is zero under forced oscillation caused by an ultrasonic wave of a specific frequency, while the other being obtained when the axial force to be measured exists under forced oscillation caused by ultrasonic wave of the same frequency.
Inventors
- 👤 Takayuki Makino
- 👤 Haruhiko Toriyama
Bibliographic Details
Application Number
—
Jurisdiction
US
Data Source
google_patents
Last Synchronized
2026-10-24 17:41
CPC Classifications
G; G01; G01L; G01L5/00; G01L5/24; G01L5/246; B; B25; B25B; B25B23/00; B25B23/14; G01H; G01H13/00; G01N; G01N29/00; G01N29/04; G01N29/12; F; F16; F16B; F16B31/00; F16B31/02; F16B2031/022; G01N2291/00; G01N2291/02; G01N2291/028; G01N2291/02827; G01N2291/26; G01N2291/269; G01N2291/2691
Claims Analysis
Total Claims: 4
Claim 1
Independent Claim
221 words
A method of obtaining a measure of an axial force within an article under strain from a variation of natural frequencies of said article, comprising the steps of: applying an ultrasonic wave to said article to generate forced oscillations therein; measuring a first natural frequency of said article when said axial force within said article is substantially zero; measuring a second natural frequency of said article when said article is under strain and said axial force is greater than zero; determining differential (f Epsilon 2-f Epsilon 1) between said first and second natural frequencies; and comparing thus determined differential with calibration data which has been obtained with respect to axial force versus differential to locate the existing axial force; the frequency of said ultrasonic wave being selected to satisfy the equation, (f Epsilon 2-f Epsilon 1)/f Epsilon 1 K(((1- Nu Epsilon 2) square root 1+ Epsilon 1/ (1- Nu Epsilon 1) square root 1+ Epsilon 2 ) -1), where f Epsilon 1 is the first measured natural frequency of said article when the strain thereof is Epsilon 1 ( Epsilon 1 > OR = 0), f Epsilon 2 is the second measured natural frequency of said article when the strain thereof is Epsilon 2 ( Epsilon 2 > 0), K is a constant greater than 3, and Nu is Poisson''s ratio.
Claim 2
Independent Claim
221 words
A method of obtaining a measure of an axial force within an article under strain from a variation of natural frequencies of said article, comprising the steps of: applying an ultrasonic wave to said article to generate forced oscillations therein; measuring a first natural frequency of said article when said axial force within said article is substantially zero; measuring a second natural frequency of said article when said article is under strain and said axial force is greater than zero; determining differential (f Epsilon 2-f Epsilon 1) between said first and second natural frequencies; and comparing thus determined differential with calibration data which has been obtained with respect to axial force versus differential to locate the existing axial force; the frequency of said ultrasonic wave being selected to satisfy the equation, (f Epsilon 2-f Epsilon 1)/f Epsilon 1 K(((1- Nu Epsilon 2) square root 1+ Epsilon 1/ (1- Nu Epsilon 1) square root 1+ Epsilon 2 ) -1), where f Epsilon 1 is the first measured natural frequency of said article when the strain thereof is Epsilon 1 ( Epsilon 1 > OR = 0), f Epsilon 2 is the second measured natural frequency of said article when the strain thereof is Epsilon 2 ( Epsilon 2 > 0), K is a constant greater than 3, and Nu is Poisson''s ratio.
Claim 3
Independent Claim
220 words
A method of obtaining a measure of an axial force within an article under strain from a variation of natural frequencies of said article, comprising the steps of: applying an ultrasonic wave to said article to generate forced oscillations therein; measuring a first natural frequency of said article when said axial force within said article is substantially zero; measuring a second natural frequency of said article when said article is under strain and said axial force is greater than zero; determining the ratio of change (f epsilon 2-f epsilon 1/f epsilon 1) between said first and second natural frequencies; and comparing thus determined ratio with calibration data which has been obtained with respect to axial force versus ratio of change; the frequency of said ultrasonic wave being selected to satisfy the equation, (f epsilon 2-f epsilon 1)/f epsilon 1 K(((1- Nu epsilon 2) Square Root 1+ epsilon 1/ (1- Nu epsilon 1) Square Root 1+ epsilon 2)-1) where f epsilon 1 is the first measured natural frequency of said article when the strain thereof is epsilon 1 ( epsilon 1 > or = 0), f epsilon 2 is the second measured natural frequency of said article when the strain thereof is epsilon 2 ( epsilon 2 > 0), K is a constant greater than 3, and Nu is Poisson''s ratio.
Claim 4
Independent Claim
220 words
A method of obtaining a measure of an axial force within an article under strain from a variation of natural frequencies of said article, comprising the steps of: applying an ultrasonic wave to said article to generate forced oscillations therein; measuring a first natural frequency of said article when said axial force within said article is substantially zero; measuring a second natural frequency of said article when said article is under strain and said axial force is greater than zero; determining the ratio of change (f epsilon 2-f epsilon 1/f epsilon 1) between said first and second natural frequencies; and comparing thus determined ratio with calibration data which has been obtained with respect to axial force versus ratio of change; the frequency of said ultrasonic wave being selected to satisfy the equation, (f epsilon 2-f epsilon 1)/f epsilon 1 K(((1- Nu epsilon 2) Square Root 1+ epsilon 1/ (1- Nu epsilon 1) Square Root 1+ epsilon 2)-1) where f epsilon 1 is the first measured natural frequency of said article when the strain thereof is epsilon 1 ( epsilon 1 > or = 0), f epsilon 2 is the second measured natural frequency of said article when the strain thereof is epsilon 2 ( epsilon 2 > 0), K is a constant greater than 3, and Nu is Poisson''s ratio.
References Cited (Backward Citations)
USPTO Annuity & Maintenance Windows
| Annuity Stage | Window Opens | Payment Deadline | Surcharge Period Until | Estimated Fee | Status |
|---|---|---|---|---|---|
| 3.5 Years (Year 4) | 1978-11-10 | 1979-05-12 | 1979-11-11 | $2000.00 | Window Closed / Lapsed |
| 7.5 Years (Year 8) | 1982-11-10 | 1983-05-12 | 1983-11-11 | $3760.00 | Window Closed / Lapsed |
| 11.5 Years (Year 12) | 1986-11-10 | 1987-05-12 | 1987-11-11 | $7700.00 | Window Closed / Lapsed |