Prosecution Insights
Last updated: April 19, 2026
Application No. 18/294,681

Method for Flow Measurement Subject to Interference, Magneto-Inductive Flow Meter and Computer Program Product

Non-Final OA §101§103
Filed
Feb 02, 2024
Examiner
NGUYEN, TRUNG Q
Art Unit
2858
Tech Center
2800 — Semiconductors & Electrical Systems
Assignee
Siemens Aktiengesellschaft
OA Round
1 (Non-Final)
91%
Grant Probability
Favorable
1-2
OA Rounds
2y 8m
To Grant
97%
With Interview

Examiner Intelligence

Grants 91% — above average
91%
Career Allow Rate
757 granted / 833 resolved
+22.9% vs TC avg
Moderate +6% lift
Without
With
+5.9%
Interview Lift
resolved cases with interview
Typical timeline
2y 8m
Avg Prosecution
31 currently pending
Career history
864
Total Applications
across all art units

Statute-Specific Performance

§101
9.7%
-30.3% vs TC avg
§103
52.4%
+12.4% vs TC avg
§102
22.1%
-17.9% vs TC avg
§112
9.7%
-30.3% vs TC avg
Black line = Tech Center average estimate • Based on career data from 833 resolved cases

Office Action

§101 §103
Notice of Pre-AIA or AIA Status The present application, filed on or after March 16, 2013, is being examined under the first inventor to file provisions of the AIA . Priority Receipt is acknowledged of certified copies of papers required by 37 CFR 1.55. Information Disclosure Statement The information disclosure statement (IDS) submitted on 03/21/2024, 02/07/2024 & 02/02/2024 are in compliance with the provisions of 37 CFR 1.97. Accordingly, the information disclosure statement is being considered by the examiner. Claim Rejections - 35 USC § 101 35 U.S.C. 101 reads as follows: Whoever invents or discovers any new and useful process, machine, manufacture, or composition of matter, or any new and useful improvement thereof, may obtain a patent therefor, subject to the conditions and requirements of this title. Claims 15–25 are rejected under 35 U.S.C. 101 because the claimed invention is directed to a judicial exception (i.e., an abstract idea) without significantly more. Claim 15 is treated as representative. Claim 15 recites, in relevant part, a method comprising: exciting a magnet coil with a square wave signal at a pulse frequency capturing a measurement signal capturing measurement value portions comprising sub portions establishing mean values of the measurement signal recognizing interference based on a difference between mean values adapting pulse duration or inactive phase to balance interference effects The limitations corresponding to recognizing interference, establishing mean values, comparing mean values, and adapting durations based on interference effects are treated as the abstract idea, while the remaining limitations are additional elements. Step 1 – Statutory Category Under Step 1 of the eligibility analysis, claim 15 is directed to a process, which is one of the four statutory categories of patent eligible subject matter. Accordingly, Step 1 is satisfied. Step 2A Prong One – Judicial Exception Under Step 2A Prong One, the claim is analyzed to determine whether it recites a judicial exception. The limitations of claim 15 directed to: establishing mean values of a measurement signal; determining whether mean values differ by at least a threshold; recognizing interference based on the comparison; adapting signal timing to balance interference; constitute an abstract idea. Under the 2019 Revised Patent Subject Matter Eligibility Guidance, these limitations fall within the groupings of: Mathematical concepts, including mathematical calculations, averaging, threshold comparison, and signal evaluation Mental processes, including observing data, comparing values, and making determinations based on the comparison Under a broadest reasonable interpretation, these steps can be performed mentally or using pen-and-paper calculations, and nothing in the claim precludes such mental performance. For example, establishing a mean value and determining whether two mean values differ by a threshold is a mathematical comparison, and recognizing interference based on that comparison is an evaluative judgment. Accordingly, claim 15 recites a judicial exception. Step 2A Prong Two – Practical Application Under Step 2A Prong Two, the claim is evaluated to determine whether it integrates the abstract idea into a practical application. The additional elements of claim 15 include: exciting a magnet coil with a square wave signal capturing a measurement signal adapting pulse duration or inactive phase These additional elements represent data acquisition and signal excitation performed using generic and conventional magneto inductive flowmeter components. Such steps merely gather data and apply the abstract idea in the context of a particular field of use, namely flow measurement. According to the October 2019 Update on Subject Matter Eligibility, data gathering and signal acquisition steps performed to supply data for abstract analysis are considered insignificant extra solution activity and do not integrate the abstract idea into a practical application. The claim does not recite any improvement to the magneto inductive flowmeter itself, nor does it recite a specific hardware configuration that changes the way the flowmeter operates at a physical level. Accordingly, claim 15 does not integrate the judicial exception into a practical application and is directed to an abstract idea. Step 2B – Significantly More Under Step 2B, the claim is evaluated to determine whether it includes additional elements that amount to significantly more than the judicial exception. Claim 15 does not include additional elements sufficient to amount to significantly more because the claimed steps of: averaging measurement signals; comparing averaged values; identifying interference; adjusting timing parameters based on the comparison are well understood, routine, and conventional in the relevant art. Strack et al. (US 2006/0028208 A1) disclose methods for measuring electromagnetic properties using conductive pipe (106)s, including: acquiring electromagnetic measurements; evaluating current leakage and electromagnetic responses; jointly processing and comparing measurement data; adjusting models and parameters based on measured interference and signal behavior. Strack et al. demonstrate that acquiring electromagnetic signals, processing them mathematically, comparing derived values, and adjusting parameters based on those comparisons were conventional techniques well known in the art prior to the effective filing date. As in the present claims, Strack et al. rely on mathematical inversion, averaging, comparison, and model based adjustment without improving the underlying electromagnetic sensing hardware itself. Accordingly, the ordered combination of steps in claim 15 amounts to nothing more than applying abstract data analysis using conventional electromagnetic measurement techniques to a particular technological environment. Claim 15 therefore does not recite significantly more than the abstract idea. Independent claim 23 recites limitations similar to claim 15 and is therefore rejected on the same grounds for being directed to an abstract idea without significantly more. Dependent Claims 16–22 & 23-24 are rejected on the same grounds as claim 15. Claims 16–18 further specify temporal relationships of measurement portions and additional averaging steps, which merely refine the mathematical analysis and do not add a practical application. Claims 19–22 recite modulation, carrier frequency comparison, and frequency shift determination, which are mathematical signal processing operations that remain within the abstract idea groupings of mathematical concepts and mental processes. Claims 23–25 recite frequency analysis, classification of frequency components, and amplitude determination, which further elaborate on mathematical analysis of signals without reciting a technological improvement to the flowmeter itself. These dependent claims merely expand the abstract idea of claims 15 & 23, which do not add meaningful limitations sufficient to integrate the abstract idea into a practical application or amount to significantly more. Claim Rejections - 35 USC § 103 The following is a quotation of 35 U.S.C. 103 which forms the basis for all obviousness rejections set forth in this Office action: A patent for a claimed invention may not be obtained, notwithstanding that the claimed invention is not identically disclosed as set forth in section 102, if the differences between the claimed invention and the prior art are such that the claimed invention as a whole would have been obvious before the effective filing date of the claimed invention to a person having ordinary skill in the art to which the claimed invention pertains. Patentability shall not be negated by the manner in which the invention was made. Claim(s) 15-30 is/are rejected under 35 U.S.C. 103 as being unpatentable over Ameri et al. (U.S. 2021/0072053 A1) in view of Almaguer (U.S. 2009/0166035 A1). Regarding claim 15, Ameri et al. disclose a method for measuring a flow rate (via sensor 108, see [0031]) in a pipe (106) via a magneto inductive flowmeter fastened to the pipe (106) (see [0036]), comprising: exciting a magnet coil (126) of the magneto inductive flowmeter with a square wave signal (168) at a pulse frequency and capturing a measurement signal (see Fig. 2 and paragraphs [0045], wherein the controller drives field coils using square wave DC excitation and captures corresponding measurement signals); capturing a first measurement value portion of the measurement signal (see paragraph [0051], wherein sampled portions of the measurement signal are captured at defined temporal locations within excitation periods); establishing a mean value of the measurement signal (see paragraph [0055], wherein multiple sampled values are averaged to establish an average measurement value). Ameri et al. fail to disclose that the measurement value portion comprises a first and a second sub portion, that an interference of the measurement signal is recognized if mean values of the first and second sub portions differ by at least an adjustable interference threshold value, and that an inactive phase of the square wave signal (168) is adjustable independently of the measurement value portion and adapted to balance an interference effect in successive measurement value portions. Almaguer disclose establishing comparative reference measurements using opposing or offset measurement points and normalizing measurement results based on differences between such measurements (see Almaguer paragraphs [0089] & [0092]), and further disclose computer controlled adjustment of excitation timing and excitation parameters to compensate for environmental and interference effects (see Almaguer paragraphs [0080] & [0110-0111]). It would have been obvious to one skilled in the art, prior to the effective filing date, to modify Ameri et al. by incorporating comparative mean based interference recognition and adaptive excitation timing as taught by Almaguer, as doing so would provide improved mitigation of interference induced measurement errors because Almaguer emphasize that excitation timing and comparative normalization compensate for environmental and electromagnetic interference effects and improve measurement accuracy (see Almaguer paragraphs [0080] & [0089]). Regarding claim 16, Ameri et al. & Almaguer disclose the method as claimed in claim 15, wherein Ameri et al. further disclose capturing measurement signal samples at different temporal locations within an excitation period and across successive excitation periods (see paragraphs [0056] & [0058], wherein sampling points are temporally offset and may partially overlap in time). PNG media_image1.png 817 1492 media_image1.png Greyscale Regarding claim 17, Ameri et al. & Almaguer disclose the method as claimed in claim 15, wherein Ameri et al. further disclose establishing a mean value of the measurement signal from sampled portions and using the established mean value to represent a magnitude of the measurement signal (see paragraph [0055], wherein averaged sampled values are used to represent signal level); establishing signal amplitude based on averaged measurement responses and calibrated signal processing (see Almaguer paragraphs [0041]). Regarding claim 18, Ameri et al. & Almaguer disclose the method as claimed in claim 16, wherein Ameri et al. further disclose establishing mean values of the measurement signal for temporally offset measurement portions (see paragraph [0055]) and determining signal magnitude based on such mean values (see [0042]). Regarding claim 19, Ameri et al. disclose performing excitation and sampling steps for successive measurement value portions (see paragraphs [0051] &[0056]). Ameri et al. fail to disclose modulating the measurement signals of the first and second measurement value portions onto a carrier signal having a carrier frequency corresponding to the pulse frequency and establishing a frequency shift relative to a comparison frequency. Almaguer disclose phase sensitive and frequency referenced signal processing synchronized to excitation timing and frequency (see Almaguer paragraphs [0088] & [0091]), which inherently requires modulation of measurement signals relative to an excitation referenced carrier and evaluation of frequency deviations. It would have been obvious to one skilled in the art, prior to the effective filing date, to modify Ameri et al. by incorporating carrier referenced modulation and frequency comparison as taught by Almaguer, as doing so would improve discrimination between interference components and excitation related signal components because Almaguer emphasize frequency and phase referenced processing to isolate interference and environmental effects (see Almaguer paragraph [0088]). Regarding claim 20, Ameri et al. & Almaguer disclose the method as claimed in claim 16, wherein Ameri et al. further disclose performing excitation and sampling for successive measurement value portions as described for claim 19 (see paragraphs [0051] & [0055]); frequency referenced and phase sensitive signal processing synchronized to excitation frequency as described above (see paragraph [0050]). Regarding claim 21, Ameri et al. & Almaguer disclose the method as claimed in claim 17, wherein Ameri et al. further disclose establishing mean values for measurement value portions and performing excitation and sampling for successive portions (see paragraph [0055]); Almaguer disclose frequency referenced processing and modulation relative to excitation timing as described above (see paragraphs [0051]). Regarding claim 22, Ameri et al. & Almaguer disclose the method as claimed in claim 19, wherein Ameri et al. further disclose that modulation onto the carrier signal occurs via quadrature amplitude modulation or that the comparison frequency is a mains target frequency (see [0054]); Almaguer disclose phase sensitive and frequency based discrimination of signals synchronized to excitation timing (see Almaguer paragraph [0052]) wherein quadrature modulation and comparison to a known reference frequency obvious signal processing techniques) Regarding claim 23, Ameri et al. disclose exciting a magnet coil (126) with a square wave signal (168) at a pulse frequency and capturing a measurement signal (see paragraphs [0036] & [0046]); performing a frequency analysis of the measurement signal to establish frequency components (see paragraph [0051], wherein sampled portions of the measurement signal are captured at defined temporal locations within excitation periods); recognizing odd numbered fractions of the pulse frequency as square wave frequency components, recognizing remaining frequency components as interference frequencies (see paragraph [0055], wherein multiple sampled values are averaged to establish an average measurement value, also see [0056]). Ameri et al. fail to disclose, adapting durations of measurement value portions and inactive phases based on interference frequency. Almaguer disclose adapting durations of measurement value portions and inactive phases based on interference frequency (see Almaguer paragraphs [0088] & [0080]). It would have been obvious to one skilled in the art, prior to the effective filing date, to modify Ameri et al. to include frequency domain classification and adaptive timing as taught by Almaguer, as doing so would allow systematic identification and suppression of interference frequencies because Almaguer emphasize frequency based characterization and compensation of electromagnetic environments (see Almaguer paragraph [0088]). Regarding claim 24, Ameri et al. & Almaguer disclose the method as claimed in claim 23, wherein Ameri et al. further disclose frequency domain analysis techniques applicable to electromagnetic measurement signals (see paragraph [0054], which rendering Fourier analysis or wavelet analysis obvious implementation choices). Regarding claim 25, Ameri et al. & Almaguer disclose the method as claimed in claim 23, wherein Ameri et al. further disclose establishing signal amplitude based on processed measurement signals (see paragraph [0055]); establishing amplitude based on frequency domain response of measurement signals (see paragraphs [0056]). Regarding claim 26, Ameri et al. disclose a control unit of a magneto-inductive flowmeter, comprising: a storage unit and a computer unit for executing a computer program product (see Ameri paragraphs [0036] and [0054], wherein a digital processor and associated memory execute control logic and signal-processing instructions); wherein the control unit is configured to excite a magnet coil of the magneto-inductive flowmeter with a square-wave signal at a pulse frequency and capture a measurement signal (see Ameri paragraphs [0036], [0045], and [0046], wherein the controller drives field coils using square-wave DC excitation and captures corresponding measurement signals); capture a first measurement value portion of the measurement signal (see Ameri paragraphs [0051] through [0056], wherein measurement signals are sampled at defined temporal locations within excitation periods); and establish a mean value of the measurement signal (see Ameri paragraph [0055], wherein multiple sampled values are averaged to establish an average measurement value). Ameri et al. fail to disclose that the measurement value portion comprises a first and a second sub-portion, that an interference of the measurement signal is recognized if mean values of the first and second sub-portions differ by at least an adjustable interference threshold value, and that a square-wave signal has an inactive phase adjustable independently of the measurement value portion, wherein at least one of a pulse duration of the square-wave signal and a duration of the inactive phase is adapted to balance an interference effect in successive measurement value portions. Almaguer disclose comparative reference-based evaluation of electromagnetic measurement signals using opposing or offset measurement points and normalization of measurement results based on differences between such measurements (see Almaguer paragraphs [0089] and [0092]), and further disclose computer-controlled adjustment of excitation timing and excitation parameters to compensate for environmental and electromagnetic interference effects (see Almaguer paragraphs [0080], [0091], [0110], and [0111]). It would have been obvious to one skilled in the art, prior to the effective filing date, to modify Ameri et al. by incorporating the comparative mean-based interference recognition and adaptive excitation timing taught by Almaguer, as doing so would provide improved mitigation of interference-induced measurement error and enhance robustness of the control unit because Almaguer emphasize that adjusting excitation timing and normalizing measurements based on comparative signal behavior compensates for environmental interference and improves accuracy of electromagnetic measurement systems (see Almaguer paragraphs [0080] and [0089]). Regarding claim 27, Ameri et al. disclose a control unit of a magneto-inductive flowmeter, comprising: a storage unit and a computer unit for executing a computer program product (see Ameri paragraphs [0036] and [0054], wherein a digital processor and associated memory execute control and signal-processing instructions); wherein the control unit is configured to excite a magnet coil of the magneto-inductive flowmeter with a square-wave signal at a pulse frequency and capture a measurement signal (see Ameri paragraphs [0036], [0045], and [0046], wherein the controller drives the field coils using square-wave DC excitation and captures corresponding measurement signals); and to perform frequency analysis of the measurement signal to establish frequency components of the measurement signal (see Ameri paragraphs [0052] through [0056], wherein sampled signals are analyzed to identify interference effects associated with excitation-related signal behavior). Ameri et al. fail to disclose recognizing a frequency component of the measurement signal as a square-wave frequency component if the frequency component corresponds to an odd-numbered fraction of the pulse frequency, recognizing other frequency components as interference frequencies, and amending durations of measurement value portions and durations of inactive phases based on a period duration of an interference frequency. Almaguer disclose frequency-domain analysis of electromagnetic measurement signals, including analysis of amplitude and phase as a function of frequency and classification of signal components relative to excitation frequency (see Almaguer paragraph [0088]), and further disclose computer-controlled adjustment of excitation parameters, including timing and frequency, based on frequency-dependent signal behavior to compensate for environmental and interference effects (see Almaguer paragraphs [0080], [0081], and [0091]). It would have been obvious to one skilled in the art, prior to the effective filing date, to modify Ameri et al. by incorporating the frequency-component classification and excitation-timing adaptation taught by Almaguer, as doing so would provide improved discrimination between excitation-related signal components and interference frequencies and allow adaptive timing control to mitigate interference effects because Almaguer emphasize that frequency-based characterization and adjustment of excitation parameters improves robustness and accuracy of electromagnetic measurement systems under varying interference conditions (see Almaguer paragraphs [0080] and [0088]). Regarding claim 28, Ameri et al. & Almaguer disclose a magneto-inductive flowmeter for measuring a flow rate through a pipe as claimed in claim 27, wherein Ameri et al. further disclose a magneto inductive flowmeter comprising magnet coils (126A-B), voltage sensors, and a control unit (see paragraphs [0035]). Regarding claim 29, Ameri et al. fail to disclose a computer program product formed as a digital twin for simulating operating behavior of a magneto inductive flowmeter. Almaguer disclose physics based electromagnetic modeling, response characterization, and computational simulation of electromagnetic tool behavior under varying operating conditions (see Almaguer paragraphs [0092], [0080] & [0081]). It would have been obvious to one skilled in the art, prior to the effective filing date, to implement such modeling as a computer program product simulating operating behavior, as doing so would enable evaluation and optimization of measurement performance under interference conditions (see Almaguer paragraphs [0092] & [0080]). Regarding claim 30, Ameri et al. fail to disclose a physics module, emulation under adjustable operating conditions including an interference spectrum, and plausibility testing of voltage sensor signals to identify a defective voltage sensor. Almaguer disclose physics based electromagnetic modeling, frequency sweeping across operating conditions, and response characterization to evaluate measurement plausibility (see Almaguer paragraphs [0081] & [0092]). It would have been obvious to one skilled in the art, prior to the effective filing date, to incorporate such physics based modeling and interference spectrum evaluation into a digital simulation to identify defective sensors, as doing so would improve diagnostic reliability of electromagnetic measurement systems (see Almaguer paragraphs [0080] & [0092]). Conclusion The prior art made of record and not relied upon is considered pertinent to applicant's disclosure. U.S. 2001/0054312 A1 to Czarnek discloses a sensor system for measuring displacement includes a primary coil wound around a longitudinal axis and at least one secondary coil wound around the longitudinal axis. Each secondary coil has a winding density distribution that varies between the ends thereof. The winding direction of each secondary coil varies between a clockwise winding direction between the ends thereof. A coupler is positioned adjacent the primary coil between the ends thereof. The coupler includes a resonating circuit configured to resonate at a resonating frequency. The coupler or the coils are configured to move relative to the other of the coupler or the coils. A control system excites the primary coil with a first step of a signal and receives from each secondary coil in response thereto a time varying signal. Each time varying signal includes a ringing component superimposed on a time varying component temporally adjacent the first step of the signal. The control system acquires plural samples of each time varying signal after the ringing component thereof dissipates and determines therefrom a position of the coupler along the longitudinal axis. U.S. 11,828,635 B2 to Forster discloses a method for operating a magnetic-inductive flowmeter includes several steps. In a calibration step, a plurality of noise-removed comparison flow measurement values are determined. A comparison frequency spectrum is determined from at least a part of a plurality of detected, noisy raw measurement signals, on which the calculation of the noise-removed comparison flow measurement values is based. In a measurement operation step, a current noise-removed flow measurement value is calculated from a plurality of detected, noisy raw measurement signals. A current measurement frequency spectrum is determined from at least some of the plurality of detected, noisy raw measurement signals. In a comparison step, the current measurement frequency spectrum is compared with one of the comparison frequency spectra and a deviation value is determined. Depending on the deviation value, the current noise-removed flow measurement value is signaled as unreliable and/or as reliable. A corresponding magnetic-inductive flowmeter is also disclosed. U.S. 2003/0029249 A1 to Keech discloses an AC electromagnetic flowmeter, a method is proposed for obtaining reliable measurement of flow across a variety of flow rates which has good stability and is immune from noise. The method comprises exciting the field generating coils of the flowmeter with an excitation signal comprising a first, relatively low frequency, component and a second, relatively high frequency, component; analyzing the induced electrode signal into a first flow measurement component generated substantially by the first excitation component and a second flow measurement component generated substantially by the second excitation component; and combining the first flow measurement component and second flow measurement component to obtain a measurement of flow based on both the first and second flow measurement components. Any inquiry concerning this communication or earlier communications from the examiner should be directed to TRUNG NGUYEN whose telephone number is (571)272-1966. The examiner can normally be reached on Mon- Friday 8AM - 4:00PM Eastern Time. If attempts to reach the examiner by telephone are unsuccessful, the examiner’s supervisor, Huy Phan can be reached on 571-272-7924. The fax phone number for the organization where this application or proceeding is assigned is 571-273-8300. Information regarding the status of an application may be obtained from the Patent Application Information Retrieval (PAIR) system. Status information for published applications may be obtained from either Private PAIR or Public PAIR. Status information for unpublished applications is available through Private PAIR only. For more information about the PAIR system, see http://pair-direct.uspto.gov. Should you have questions on access to the Private PAIR system, contact the Electronic Business Center (EBC) at 866-217-9197 (toll-free). If you would like assistance from a USPTO Customer Service Representative or access to the automated information system, call 800-786-9199 (IN USA OR CANADA) or 571-272-1000. Examiner: /Trung Q. Nguyen/- Art 2858 January 6, 2026 /HUY Q PHAN/ Supervisory Patent Examiner, Art Unit 2858
Read full office action

Prosecution Timeline

Feb 02, 2024
Application Filed
Jan 06, 2026
Non-Final Rejection — §101, §103
Apr 07, 2026
Response Filed

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Prosecution Projections

1-2
Expected OA Rounds
91%
Grant Probability
97%
With Interview (+5.9%)
2y 8m
Median Time to Grant
Low
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