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Dive into the research topics where Robert W. Brumley is active.

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Featured researches published by Robert W. Brumley.


Classical and Quantum Gravity | 2015

The Gravity Probe B test of general relativity

C.W.F. Everitt; Barry Muhlfelder; D. DeBra; Brad Parkinson; John P. Turneaure; A S Silbergleit; E B Acworth; M Adams; Ronald J. Adler; William J. Bencze; J E Berberian; R J Bernier; K A Bower; Robert W. Brumley; Sasha Buchman; K Burns; B. Clarke; John Conklin; M L Eglington; G Green; Gregory M. Gutt; D H Gwo; G Hanuschak; X He; M I Heifetz; David Hipkins; T. Holmes; R A Kahn; G. M. Keiser; J. Kozaczuk

The Gravity Probe B mission provided two new quantitative tests of Einsteins theory of gravity, general relativity (GR), by cryogenic gyroscopes in Earths orbit. Data from four gyroscopes gave a geodetic drift-rate of −6601.8 ± 18.3 marc-s yr−1 and a frame-dragging of −37.2 ± 7.2 marc-s yr−1, to be compared with GR predictions of −6606.1 and −39.2 marc-s yr−1 (1 marc-s = 4.848 × 10−9 radians). The present paper introduces the science, engineering, data analysis, and heritage of Gravity Probe B, detailed in the accompanying 20 CQG papers.


The second international laser interferometer space antenna symposium (LISA) on the detection and observation of gravitational waves in space | 1998

The design and testing of the Gravity Probe B suspension and charge control systems

Saps Buchman; William J. Bencze; Robert W. Brumley; Bruce Clarke; G. M. Keiser

The Relativity Mission Gravity Probe B (GP-B), is designed to verify two rotational effects predicted by gravitational theory. The GP-B gyroscopes (which also double as drag free sensors) are suspended electrostatically, their position is determined by capacitative sensing, and their charge is controlled using electrons generated by ultraviolet photoemission. The main suspension system is digitally controlled, with an analog backup system. Its functional range is 10 m/s2 to 10−7 m/s2. The suspension system design is optimized to be compatible with gyroscope Newtonian drift rates of less than 0.1 marcsec/year (3×10−12 deg/hr), as well as being compatible with the functioning of an ultra low noise dc SQUID magnetometer. Testing of the suspension and charge management systems is performed on the ground using flight gyroscopes, as well as a gyroscope simulator designed to verify performance over the entire functional range. We describe the design and performance of the suspension, charge management, and gyros...


Advances in Space Research | 2000

Gyroscopes and charge control for the Relativity Mission Gravity Probe B

Saps Buchman; C.W.F. Everitt; Brad Parkinson; John P. Turneaure; Robert W. Brumley; Dale Gill; G. M. Keiser; Y.M. Xiao

The most demanding goal of the Gravity Probe B Relativity Mission (GP-B) is the measurement of the parametrized post-Newtonian parameter γ to one part in 105. This goal requires a total experimental accuracy of ≤ 0.044 marcsec/yr. Analysis of and results from 100,000 hours of gyroscope operation on the ground show that the residual Newtonian drift will be < 0.17 marcsec/yr for a supported gyroscope in 10−9 m/s2, and < 0.020 marcsec/yr for an unsupported gyroscope in a fully inertial orbit. The expected error due to gyroscope drift is thus consistent with the measurement goal. The main gyroscope disturbance caused by cosmic radiation is charging of the rotor. A force modulation technique allows measurement of the charge of the gyroscope rotor to about 5 pC, while bipolar charge control to 10 pC is achieved using electrons generated by UV photoemission.


Classical and Quantum Gravity | 2015

The Gravity Probe B electrostatic gyroscope suspension system (GSS)

William J. Bencze; Robert W. Brumley; M L Eglington; David Hipkins; T. Holmes; Brad Parkinson; Y Ohshima; C.W.F. Everitt

A spaceflight electrostatic suspension system was developed for the Gravity Probe B (GP-B) Relativity Missions cryogenic electrostatic vacuum gyroscopes which serve as an indicator of the local inertial frame about Earth. The Gyroscope Suspension System (GSS) regulates the translational position of the gyroscope rotors within their housings, while (1) minimizing classical electrostatic torques on the gyroscope to preserve the instruments sensitivity to effects of General Relativity, (2) handling the effects of external forces on the space vehicle, (3) providing a means of precisely aligning the spin axis of the gyroscopes after spin-up, and (4) acting as an accelerometer as part of the spacecrafts drag-free control system. The flight design was tested using an innovative, precision gyroscope simulator Testbed that could faithfully mimic the behavior of a physical gyroscope under all operational conditions, from ground test to science data collection. Four GSS systems were built, tested, and operated successfully aboard the GP-B spacecraft from launch in 2004 to the end of the mission in 2008.


Czechoslovak Journal of Physics | 1996

Measurements of the thermal emissivity of a superconducting niobium film

Robert W. Brumley; Saps Buchman; John Mester

The radiative exchange of heat between a superconducting Nb film at 4.2 K and a Ti film at 4.2-11 K has been measured. A Nb-coated quartz sphere was used as a bolometer to measure total heat absorbed, from which an effective emissivity was derived. Under these conditions the effective emissivity of the Nb film is about 3%.


Classical and Quantum Gravity | 1996

Experimental techniques for gyroscope performance enhancement for the Gravity Probe B relativity mission

Saps Buchman; Francis Everitt; Brad Parkinson; John P. Turneaure; Mac Keiser; M. A. Taber; Doron Bardas; J.M. Lockhart; Barry Muhlfelder; John Mester; Yueming Xiao; Gregory M. Gutt; Dale Gill; Robert W. Brumley; Brian DiDonna

The Gravity Probe B relativity mission experiment is designed to measure the frame dragging and geodetic relativistic precessions in a 650 km polar orbit. We describe some of the advanced experimental techniques used to achieve the required gyroscope accuracy of between 0.05 and . The subjects discussed are: (i) the development of high-precision gyroscopes with drift rates of less than , (ii) a low-temperature bake-out procedure resulting in a helium pressure of less than at 2.5 K, (iii) a read-out system using DC SQUID magnetometers with a noise figure of at 5 mHz and (iv) AC and DC magnetic shielding techniques which produce an AC attenuation factor in excess of and a residual DC field of less than .


Physica B-condensed Matter | 1994

Trapped flux reduction in a spherical niobium shell at 1 mG

Robert W. Brumley; Saps Buchman; Yueming Xiao

Abstract We have developed a method to reduce flux trapped in a superconducting spherical shell. A normal spot on the shell sweeps flux lines until they close in on themselves. Using this technique the dipole moment corresponding to a trapped field of 1 mG has been reduced to about 6% of its original level.


Archive | 2005

Methods and apparatus for a navigation system with reduced susceptibility to interference and jamming

Clark E. Cohen; Robert W. Brumley; Mark L. Psiaki; Gregory M. Gutt; William J. Bencze; Brent M. Ledvina; Barton G. Ferrell; David A. Whelan


Archive | 2009

Precise Absolute Time Transfer From A Satellite System

Clark E. Cohen; David A. Whelan; Robert W. Brumley; Gregory M. Gutt; Barton G. Ferrell


Archive | 2007

Generalized high performance navigation system

Clark E. Cohen; David A. Whelan; Robert W. Brumley; Gregory M. Gutt; Barton G. Ferrell

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