Ballistic galvanometer

Ballistic galvanometerMain

Community hub

8 pages, 0 posts

0 subscribers

Recent from talks

Be the first to start a discussion here.

Recent from talks

Be the first to start a discussion here.

Contribute something

About hubMembersContent overviewUpdatesRules

Main reference articles

Ballistic galvanometer

View on Wikipedia

from Wikipedia

A ballistic galvanometer is a type of sensitive galvanometer; commonly a mirror galvanometer. Unlike a current-measuring galvanometer, the moving part has a large moment of inertia, thus giving it a long oscillation period. It is really an integrator measuring the quantity of charge discharged through it. It can be either of the moving coil or moving magnet type.

Before first use the ballistic constant of the galvanometer must be determined. This is usually done by connecting to the galvanometer a known capacitor, charged to a known voltage, and recording the deflection. The constant K is calculated from the capacitance C, the voltage V and the deflection d: $K=CV/d$

where K is expressed in coulombs per centimeter.

In operation the unknown quantity of charge Q (in coulombs) is simply: $Q=kd$ .

Grassot Fluxmeter

[edit]

The Grassot Fluxmeter solves a particular problem encountered with regular galvanometers. For a regular galvanometer, the discharge time must be shorter than the natural period of oscillation of the mechanism. In some applications, particularly those involving inductors, this condition cannot be met. The Grassot fluxmeter resolves this problem, by operating without any restoring force, making the oscillation period effectively infinite and thereby longer than any discharge time.

Its construction is similar to that of a ballistic galvanometer, but its coil is suspended without any restoring forces in the suspension thread or in the current leads. The core (bobbin) of the coil is of a non-conductive material. When an electric charge is connected to the instrument, the coil starts moving in the magnetic field of the galvanometer's magnet, generating an opposing electromotive force and coming to a stop regardless of the time of the current flow. The change in the coil position is proportional only to the quantity of charge. The coil is returned to the zero position manually or by reversing the direction of the current.

References

[edit]

Wikimedia Commons has media related to Ballistic galvanometers.

Earle Terry, Advanced Laboratory Practice in Electricity and Magnetism. McGraw-Hill, New York 1929 Page 24-34
Electrical Instruments, "Tylor-Cambridge", Cambridge Scientific Instrument Company, Trade catalog, 1908 Page 34
Bakshi, U.A. and Bakshi, L.A.V., Electronic Measurements and Instrumentation, Technical Publications, 2020, Chapter 2
Bakshi, U.A. and Bakshi, L.A.V., Electric Measurements and Instrumentation, Technical Publications, 2020, Chapter 2

Revisions and contributors Edit on Wikipedia Read on Wikipedia

View on Grokipedia

from Grokipedia

A ballistic galvanometer is a type of sensitive electromagnetic instrument, typically employing a moving coil suspended in a magnetic field, designed to measure the total quantity of electric charge (Q) that passes through it during a short-duration impulse, rather than a steady current, by recording the maximum angular deflection or "throw" of its moving coil. Unlike standard galvanometers, it features a coil with a large moment of inertia and low damping to allow the moving system to swing freely, ensuring the first maximum deflection is directly proportional to the charge impulse ∫i dt. This design enables precise quantification of transient electrical events, such as those arising from sudden changes in magnetic flux according to Faraday's law of electromagnetic induction.^[1] The principle of operation relies on the equation of motion for the coil: K d²θ/dt² + D dθ/dt + Uθ = G i(t), where K is the moment of inertia, D is the damping coefficient, U is the torsional restoring constant, G is the galvanometer constant, i(t) is the instantaneous current, and θ is the angular deflection; for ballistic use with a short current pulse, the impulse approximation yields a first maximum deflection proportional to the total charge Q, with the system tuned for a long period T_b = 2π √(K/U) typically around 2 seconds to maximize sensitivity S_q = G / √(K U).^[2] Calibration relates the observed deflection to charge via Q = (N A ΔB)/R for flux-linked applications, where N is the number of turns, A is the coil area, ΔB is the change in magnetic induction, and R is the circuit resistance.^[1] Developed in the early 19th century by French physicist Claude Servais Pouillet as an advancement in electromagnetic measurement, it addressed the need for detecting brief currents beyond the capabilities of earlier tangent galvanometers.^[3] In practice, ballistic galvanometers are integral to magnetic measurements, often paired with a flip coil or Rowland ring: when the coil is rapidly rotated in a magnetic field B or the field is varied, the induced emf drives a charge pulse through the galvanometer, allowing determination of flux density or material permeability with high accuracy.^[1] They have been employed in standards laboratories for calibrating magnetic fields and in experiments like the Rowland ring method, where a secondary winding detects flux changes in toroidal samples to compute magnetic induction variations ΔB = (R Δq)/(N A).^[1] While largely superseded by digital fluxmeters in modern applications, their elegant mechanical sensitivity remains a cornerstone in the history of electrical metrology.^[2]

History and Development

Invention and Early Contributions

The galvanometer originated from the work of Johann Schweigger, who in 1820 constructed the first device capable of amplifying the deflection of a magnetic needle caused by electric currents, serving as a multiplier for voltaic electricity detection.^[4] This invention built directly on Hans Christian Ørsted's 1820 observation of electromagnetic deflection and marked the initial step toward quantitative electrical measurements.^[5] In the early 1820s, André-Marie Ampère advanced the instrument's design by incorporating mathematical formulations to enhance its sensitivity for detecting steady currents, establishing foundational principles for electromagnetic detection that extended to transient phenomena.^[5] Ampère's refinements addressed the need for more precise current quantification, influencing subsequent adaptations for impulse-based applications. The conceptual application of ballistic principles to galvanometers emerged around the 1840s, primarily to overcome the shortcomings of steady-state meters in handling brief electric charge impulses, such as those from electrostatic discharges. French physicist Claude Servais Mathias Pouillet invented the ballistic galvanometer circa 1844, adapting the device to measure the total quantity of electricity passing through it in short durations by observing the initial "throw" of the needle proportional to the charge.^[6] This innovation proved essential for experiments involving capacitor discharges and rapid transients, where traditional galvanometers failed to capture integrated charge effectively. William Thomson (later Lord Kelvin), in his early research during the 1840s and 1850s, explored similar impulse measurement techniques, culminating in his 1858 patent for the sensitive mirror galvanometer, which amplified ballistic-like responses for practical use in telegraphy and electrostatic studies.^[7]

Evolution in the 19th and 20th Centuries

In the mid-19th century, significant improvements to the ballistic galvanometer were made by James Clerk Maxwell, who in 1865 introduced a ballistic deflection method utilizing the instrument to measure inductance in electromagnetic induction experiments. This approach built on earlier discoveries of self-induction by Michael Faraday and Joseph Henry, adapting the galvanometer's response to transient currents for precise quantification of magnetic effects in circuits. Maxwell's method involved balancing the time constant of an inductive circuit against a known capacitive one, enhancing the instrument's utility in verifying Faraday's laws of induction. By the late 19th century, the ballistic galvanometer saw further developments in its application for precise charge measurement through integration with capacitor discharge techniques. This method, practically refined by Maxwell in 1865 and others in subsequent decades, involved charging a known capacitor and discharging it through the galvanometer to determine capacitance or charge quantity based on the first swing deflection.^[8] These advancements allowed for absolute measurements of electrical capacity, supporting growing needs in telegraphy and early electrical engineering. The instrument's adoption in international standards for electrical units occurred during the 1881 International Electrical Congress in Paris, where the names ampere, ohm, and coulomb were adopted, and absolute (centimeter-gram-second) units were recommended for electrical quantities. While practical international definitions were established later at the 1893 Chicago Congress, the 1881 event influenced metrology by endorsing absolute determination methods, some of which relied on galvanometers for verifying quantities of electricity. In the early 20th century, enhancements focused on improving mechanical stability, with Émile Grassot developing the fluxmeter around 1908–1910—a specialized ballistic galvanometer featuring advanced suspension systems using quartz fibers and minimized electromagnetic damping to achieve near-zero restoring torque. This design allowed for more accurate integration of flux changes over time, reducing errors from oscillatory motion and enabling finer measurements in magnetic field studies. The ballistic galvanometer's prominence began to decline after the 1950s with the rise of electronic alternatives like integrating amplifiers and cathode-ray oscilloscopes, which offered greater speed and precision without mechanical inertia. Despite this, it persisted in specialized physics laboratories for calibration and low-noise charge measurements into the 1970s, until digital oscilloscopes and data acquisition systems fully supplanted it in most applications.

Principle of Operation

Fundamental Concept

A ballistic galvanometer is a highly sensitive instrument, based on the moving-coil design, that measures the total quantity of electric charge passing through it over a very short duration, distinguishing it from standard galvanometers which are suited for steady currents.^[9]^[1] The core principle involves the coil, suspended in a uniform magnetic field, experiencing a torque when a sudden pulse of current flows through it due to the interaction between the current and the field.^[9]^[10] This torque imparts an angular impulse to the coil, analogous to a ballistic trajectory, resulting in a rapid deflection or "throw" followed by oscillation, where the amplitude of this initial swing is directly proportional to the total charge Q.^[1]^[10] In contrast to steady-state galvanometers that use significant damping to achieve a stable pointer position, the ballistic galvanometer employs zero or minimal damping to permit the coil to oscillate freely after the impulse, ensuring that the maximum deflection accurately reflects the impulsive charge without interference from rapid settling.^[9]^[1] This design leverages the fundamental physics of electromagnetic torque on a current-carrying loop, converting the brief charge flow into measurable mechanical motion for precise quantification in transient electrical events.^[9]^[10]

Mathematical Theory and Equations

The mathematical theory of the ballistic galvanometer centers on the angular impulse delivered to the coil by a transient charge and the resulting oscillatory motion, which allows the total charge to be determined from the maximum deflection. When a total charge

Q

flows through the coil over a short duration

\Delta t \ll T

, where

T

is the natural period of oscillation, the angular impulse is

N B A Q

, with

N

the number of turns in the coil,

B

the magnetic field strength, and

A

the effective area of the coil.^[11] This impulse equals the initial angular momentum of the moving system, given by

I \left. \frac{d\theta}{dt} \right|_{t=0} = N B A Q

Idtdθ

t=0=NBAQ, where $I$ is the moment of inertia about the suspension axis.^[12] In the undamped approximation, the equation of motion following the impulse is $I \frac{d^2 \theta}{dt^2} + k \theta = 0$ , where $k$ is the torsional constant of the suspension, with initial conditions $\theta(0) = 0$ and $\frac{d\theta}{dt}(0) = \frac{N B A Q}{I}$ . The solution is simple harmonic motion $\theta(t) = \theta_\mathrm{max} \sin(\omega t)$ , where the angular frequency $\omega = \sqrt{k / I}$

and the maximum deflection $\theta_\mathrm{max} = \frac{N B A Q}{\sqrt{I k}}$

NBAQ.^[11] The period is $T = 2\pi \sqrt{I / k}$

, so rearranging yields the charge-deflection relation $Q = \frac{\theta_\mathrm{max} k T}{2\pi N B A}$ , showing that $\theta_\mathrm{max} \propto Q / T$ .^[12] This derivation assumes a sudden discharge ( $\Delta t \ll T$ ), negligible damping, and measurement of the first half-period swing to capture $\theta_\mathrm{max}$ . In reality, damping introduces errors, governed by the full equation of motion $I \frac{d^2 \theta}{dt^2} + c \frac{d\theta}{dt} + k \theta = 0$ , where $c$ is the damping coefficient. For small damping, the observed first deflection $\theta_1$ underestimates the undamped value, requiring a correction factor of approximately $1 + \frac{\lambda}{2}$ to obtain the true charge, with $\lambda$ the logarithmic decrement determined from successive swings as $\lambda = \ln(\theta_1 / \theta_2)$ .^[13]

Construction and Design

Key Components

The ballistic galvanometer consists of several essential physical components designed to facilitate the precise measurement of electric charge by converting transient current impulses into observable mechanical oscillations. These components work together to produce a torque on the coil in response to charge flow, allowing the initial deflection amplitude to be proportional to the total charge passed.^[9] The moving coil is a critical element, typically rectangular or circular and wound with fine copper wire on a non-conducting frame such as plastic or bakelite, featuring 100-200 turns to enhance sensitivity and generate a sufficient magnetic moment. This construction provides a high moment of inertia, achieved by the coil's size and sometimes additional attached masses, which ensures sustained oscillations after the impulse, enabling accurate integration of the charge over time without rapid decay. The role of the coil is to interact with the magnetic field, producing a deflecting torque proportional to the charge, as the current impulse causes it to rotate briefly.^[12]^[14]^[15] Permanent magnets, often in a horseshoe configuration with concave pole pieces, generate a strong and uniform radial magnetic field across the coil, typically in the range of 0.1-0.5 T to ensure consistent torque production regardless of the coil's angular position. This radial field design minimizes restoring torque variations, allowing the coil to experience a pure deflecting force from the charge-induced current, which is essential for ballistic charge quantification. A soft iron core may be placed inside the coil to concentrate and uniformize the field lines further.^[11]^[16] The suspension system employs a thin phosphor bronze strip or quartz fiber to support the coil, offering a low torsional constant (around 10^{-6} to 10^{-5} Nm/rad) and minimal friction to permit nearly frictionless rotation. This setup allows the coil to oscillate freely with minimal energy loss, preserving the initial "throw" deflection that directly corresponds to the passed charge, while avoiding external disturbances.^[12]^[15]^[9] A lightweight mirror is attached directly to the moving coil or its suspension, enabling optical magnification of the deflection by reflecting a light beam onto a distant scale, often several meters away, for precise reading of the oscillation amplitude. This component enhances readability and accuracy in charge measurement by projecting the coil's motion without mechanical pointers that could add inertia.^[9]^[12] The frame and damping control utilize a non-magnetic aluminum structure to house the assembly, preventing interference with the magnetic field, while damping mechanisms—such as adjustable air vanes or electromagnetic setups—are configured to near-zero levels for ballistic operation. This low damping ensures the coil performs undamped or lightly damped harmonic motion, where the first half-period swing amplitude accurately reflects the total charge without significant energy dissipation.^[9]^[15]^[14]

Special Design Features for Ballistic Measurement

The ballistic galvanometer is distinguished from standard galvanometers by several specialized design modifications that optimize its response to transient impulses, such as short bursts of charge, allowing for precise measurement of the total quantity of electricity passed rather than steady currents. A primary feature is the high moment of inertia of the moving coil system, achieved through the use of a larger coil or additional masses attached to the frame, which results in a long oscillation period—typically on the order of several seconds—enabling accurate observation and measurement of the initial swing amplitude without interference from subsequent oscillations.^[11]^[17] To ensure the coil performs a near-undamped "ballistic throw," minimal damping is incorporated via a loose suspension, often using thin phosphor bronze strips or quartz fibers, combined with controlled air resistance and avoidance of metallic frames that could induce eddy currents. This design keeps the damping coefficient low, with a damping factor typically less than 0.1, preventing rapid decay of the oscillation and preserving the impulse's full effect for reliable first-swing deflection readings.^[9]^[12]^[18] The magnetic field is configured as a uniform radial field to maintain consistent torque during the coil's swing, achieved with concave or specially shaped pole pieces that keep the field lines perpendicular to the plane of the coil throughout its deflection, thereby minimizing variations in the restoring torque. An optional soft iron core may be placed within the coil to concentrate the magnetic flux, enhancing sensitivity for weaker impulses.^[19]^[20]^[21] Sensitivity to varying charge magnitudes is adjusted by incorporating variable resistance in the external circuit, allowing the total circuit resistance to be tuned for optimal deflection without overloading the instrument. For protection against accidental high steady currents that could damage the coil, shunt circuits are included in parallel, diverting excess current while permitting normal ballistic operation.^[12]

Operation and Calibration

Measurement Procedure

To measure charge using a ballistic galvanometer, the instrument must first be prepared by ensuring it is at rest with the light spot aligned at zero on the scale. The galvanometer is connected in series with the circuit containing the charge source, such as a capacitor, and a switch mechanism designed for rapid, momentary closure to enable sudden discharge. The setup includes a lamp and scale arrangement for precise deflection reading, with the galvanometer leveled to avoid external influences like vibrations or magnetic fields. Low-resistance, insulated connecting wires are used to minimize losses.^[22]^[23] The impulse is applied by charging the capacitor to a known voltage using a DC source and rheostat, then abruptly discharging the charge

Q

through the galvanometer coil by closing the switch for a very short duration, typically much less than the instrument's period of oscillation. This creates a transient current pulse that imparts angular momentum to the coil without sustained flow. The maximum deflection

\theta

of the first throw is theoretically proportional to

Q

.^[9]^[23] Observation involves illuminating the mirror attached to the coil with a lamp, projecting the reflected beam onto a distant scale to measure the peak displacement of the first swing in millimeters (or converted to radians for analysis). The coil must be allowed to come to rest naturally after each throw, often using a damping key only when the spot crosses zero to avoid interference.^[24]^[25] For accuracy, the discharge process is repeated several times (at least five trials), and the average

\theta

is computed to mitigate random variations from factors like residual charge or mechanical inconsistencies. If electromagnetic or air damping is present, a ballistic correction factor is applied to adjust the observed deflection, accounting for energy loss during the initial swing. Between trials, the capacitor is fully discharged, and the galvanometer coil is rested to prevent thermal buildup.^[22]^[26] Data recording includes noting the average

\theta

, along with environmental conditions such as ambient temperature, which can affect the torsional elasticity of the suspension fiber and thus the deflection sensitivity. Stable room conditions are maintained to ensure consistency.^[23]^[27]

Calibration Techniques

Calibration of a ballistic galvanometer involves determining its charge sensitivity constant, typically denoted as

S

, which relates the total charge

Q

passing through the instrument to the observed first throw deflection

\theta

via

S = Q / \theta

. This constant ensures accurate quantitative measurements of charge impulses, and calibration must account for the instrument's undamped oscillatory response.^[28] One primary method employs a standard capacitor to deliver a known charge impulse. A capacitor of known capacitance

C

is charged to a precisely measured voltage

V

, yielding a charge

Q = C V

. This capacitor is then rapidly discharged through the galvanometer circuit using a double-throw switch, and the resulting first maximum deflection

\theta

is recorded. The sensitivity is calculated as

S = C V / \theta

. To minimize errors from residual magnetism or asymmetry, discharges are performed with reversed polarities, and deflections are averaged over multiple trials with varying

C

and

V

values. A linear plot of

\theta

versus

C V

confirms the constant

S

. This technique is straightforward and suitable for laboratory settings where standard capacitors are available.^[28] Another established approach utilizes mutual inductance to generate a controlled flux impulse. A primary coil with known mutual inductance

M

to a secondary coil (connected to the galvanometer) carries a steady current

I

, which is suddenly reversed or interrupted using a commutator or switch. The induced charge in the secondary circuit is

Q = M \Delta I / R

, where

\Delta I

is the change in primary current and

R

is the total resistance in the secondary circuit (including a current-limiting resistor). The deflection

\theta

is measured, allowing computation of

S = (M \Delta I / R) / \theta

. Calibration currents are typically adjusted to produce deflections around 10 cm for optimal sensitivity, and multiple reversals establish consistent results. This method is particularly valuable for magnetic flux measurements, as it aligns with the galvanometer's typical applications.^[29]^[30] Calibration is generally performed immediately before each experiment to account for potential drifts. Factors such as mechanical aging of the suspension fibers or thermal variations in the coil can alter the sensitivity over time, necessitating periodic re-verification, often monthly for frequently used instruments. To minimize errors in quantitative readings, the galvanometer's natural period

T

is measured to ensure the impulse duration is much shorter than

T/4

, and the ballistic reduction factor—accounting for partial damping during the first swing—is applied as a correction multiplier, typically close to 1 for low-damping designs. These steps enhance precision to within 0.1-1% depending on setup quality.^[28]^[30]

Applications and Uses

In Physics and Electrical Experiments

The ballistic galvanometer plays a key role in laboratory experiments for determining the capacitance of a capacitor by quantifying the electric charge stored on it. In a typical procedure, a capacitor is charged to a known potential difference

V

using a battery or power supply, then rapidly discharged through the galvanometer coil. The resulting "throw" or maximum deflection

\theta

of the coil is proportional to the total charge

Q

passing through it, as

Q = k \theta

, where

k

is the instrument's charge constant determined via prior calibration. Since the charge on the capacitor is given by

Q = C V

, the capacitance

C

can be calculated as

C = Q / V

, providing a direct verification of this fundamental relation in electrostatics.^[31]^[32] This instrument is also employed to verify the principle of charge conservation in electrostatic experiments involving charge sharing between capacitors. For instance, a single capacitor is charged to a fixed voltage and discharged through the ballistic galvanometer, yielding a deflection

\theta_1

proportional to its charge

Q_1 = C V

. Two identical capacitors are then connected in parallel, charged to the same voltage, and discharged together, producing a deflection

\theta_2 \approx 2 \theta_1

, confirming that the total charge

Q_2 = 2 Q_1

is conserved during the sharing process without loss. Such demonstrations illustrate the additivity of capacitances in parallel configurations while upholding charge invariance.^[33] In measurements of high resistances, the ballistic galvanometer utilizes the leakage method to assess values typically exceeding megohms, where steady-state current methods are insensitive. A known capacitor is charged to a fixed voltage and then connected across the unknown high resistance

R

, allowing charge to leak gradually; after a measured time interval

t

, the remaining charge is discharged through the galvanometer, and the deflection indicates the leaked quantity. The resistance is derived from the exponential decay,

Q(t) = Q_0 e^{-t / ([R](/page/R) C)}

, where

C

is the capacitor's capacitance, enabling precise determination of

R

from successive deflection ratios.^[18] The ballistic galvanometer serves as an absolute standard for calibrating electrometers in experiments involving ion collection, such as those measuring ionization from radiation sources. By discharging a known capacitor through the galvanometer to establish a reference charge

Q

, the deflection provides a traceable quantity that sets the electrometer's scale for detecting small charges accumulated on electrodes from ion fluxes, ensuring accuracy in quantitative electrostatic assessments.^[34] A notable historical application occurred in the 19th century, where the ballistic galvanometer was instrumental in verifying Faraday's laws of electrolysis. Michael Faraday employed it to measure the total charge passed through electrolytic cells during decomposition, demonstrating that the mass of substance deposited or liberated at an electrode is directly proportional to the quantity of electricity

Q

(first law) and inversely proportional to its equivalent weight (second law), with deflections quantifying

Q

for precise correlations between charge and chemical yields.^[35]

In Magnetic and Flux Measurements

The ballistic galvanometer plays a crucial role in magnetic and flux measurements by quantifying transient charges induced by sudden changes in magnetic flux, leveraging its sensitivity to integrate electromagnetic induction effects over short durations. This capability stems from its design to measure total charge passed through the coil rather than steady currents, making it ideal for experiments involving flux linkages in inductive setups./10%3A_Electromagnetic_Induction/10.04%3A_Ballistic_Galvanometer_and_the_Measurement_of_Magnetic_Field) In the measurement of mutual inductance between two coils, a sudden change in current in the primary coil induces a flux linkage in the secondary coil, connected to the ballistic galvanometer via a known resistance. The resulting charge

Q

in the secondary circuit is given by

Q = \frac{M \Delta I}{R}

, where

M

is the mutual inductance,

\Delta I

is the change in primary current, and

R

is the total resistance of the secondary circuit. The galvanometer's first throw deflection

\theta

is proportional to

Q

, allowing

M

to be determined after calibration, typically by comparing to a known steady deflection. This method provides precise values for

M

in the range of millihenries, essential for verifying inductive coupling in electromagnetic devices.^[36] For determining the horizontal component

B_h

of Earth's magnetic field, a flip coil (or earth inductor) with

N

turns and area

A

is oriented parallel to the magnetic meridian and rapidly rotated 180° in the horizontal plane. This rotation changes the flux linkage by

2 N A B_h

, inducing a charge

Q = \frac{2 N A B_h}{R}

in the circuit connected to the ballistic galvanometer, where

R

is the total resistance. The deflection

\theta

relates to

Q

via the galvanometer constant, yielding

B_h = \frac{\theta k R}{2 N A}

, with

k

determined from calibration using a known field from a Helmholtz coil. Typical values obtained are around 20–30 μT, aligning with global geomagnetic surveys.^[29] The magnetic moment

m

of a bar magnet is measured using a search coil connected to the ballistic galvanometer, where the coil is placed perpendicular to the magnet's axis and the magnet is suddenly inserted or flipped to induce a flux change. The flux

\Phi

through the coil due to the dipole field is approximately

\Phi = \frac{\mu_0}{4\pi} \frac{2 m N A}{d^3}

, where

d

is the distance from the magnet's center,

N

and

A

are the coil's turns and area, and

\mu_0

is the permeability of free space; the induced charge

Q = \frac{\Delta \Phi}{R}

produces a deflection proportional to

m

. This setup allows computation of

m

for typical bar magnets on the order of 0.1–1 A·m², providing insights into material magnetization.^[37] In tracing magnetic hysteresis loops, the ballistic galvanometer integrates flux changes in a Rowland ring setup, where the ring's secondary winding is connected in series with the galvanometer and a mutual inductor for calibration. The primary coil is energized to set the magnetizing field

H

, and sudden reversals of current produce deflections corresponding to flux density

B

changes via

\Delta \Phi = N A \Delta B

, with

Q = \frac{\Delta \Phi}{R}

; repeated steps at varying

H

plot the loop, revealing coercivity and remanence. This ballistic method, though stepwise, accurately captures loop areas for soft magnetic materials.^[38] Historically, in 20th-century geophysics, the ballistic galvanometer facilitated paleomagnetism studies by measuring induced charges from flux changes during sample demagnetization impulses. For instance, Raymond Chevallier's 1925 analysis of Etna lavas used a mobile search coil setup with the galvanometer to quantify remanent magnetization directions, achieving accuracies better than 2° and revealing declination variations over centuries. This approach supported early reconstructions of geomagnetic field behavior in volcanic rocks.^[39]

Comparison with Moving-Coil Galvanometer

The ballistic galvanometer and the moving-coil galvanometer, while sharing basic components such as a coil suspended in a magnetic field, differ fundamentally in their operational principles and applications. The ballistic galvanometer is designed to measure the total charge Q passed through it in a short impulse, where the maximum deflection of the first swing is proportional to Q, making it ideal for transient phenomena like capacitor discharges. In contrast, the moving-coil galvanometer measures steady currents I, with deflection directly proportional to I, suited for continuous DC measurements. A key distinction lies in their damping mechanisms. The ballistic galvanometer employs minimal or zero damping to allow the coil to oscillate freely after an impulse, enabling observation of the initial swing amplitude without rapid decay. The moving-coil galvanometer, however, incorporates critical damping to ensure the pointer settles quickly to its final position without overshooting, facilitating accurate readings of steady-state deflections. In terms of sensitivity, the ballistic galvanometer excels at detecting small transient charges, capable of resolving quantities on the order of microcoulombs due to its undamped oscillatory response. The moving-coil galvanometer, optimized for sustained currents, is more sensitive to microampere-level steady flows but less effective for brief pulses. Response times also vary significantly: the ballistic galvanometer relies on capturing the first swing, which typically occurs over seconds, to quantify the impulse. The moving-coil galvanometer provides a steady pointer reading in milliseconds, allowing for rapid, repeated measurements of ongoing currents. These differences impose specific limitations. The ballistic galvanometer is unsuitable for direct current (DC) measurements, as its undamped oscillations would not stabilize for steady inputs. Conversely, the moving-coil galvanometer is insensitive to very fast pulses, often missing transient charges that the ballistic type can detect.

Grassot Fluxmeter as a Variant

The Grassot fluxmeter is an aperiodic variant of the ballistic galvanometer, invented by French engineer Émile Grassot in 1904.^[40] Designed specifically for precise magnetic flux measurements, it operates without a restoring torque, relying instead on its exceptionally high moment of inertia to achieve a stable, proportional deflection that directly corresponds to changes in magnetic flux. This eliminates the oscillatory behavior typical of standard ballistic instruments, making it ideal for integrating flux over time.^[41]^[42] A defining feature is the fluxmeter constant

K

, which relates the instrument's deflection

\phi

linearly to the total magnetic flux

\Phi = \int \mathbf{B} \cdot d\mathbf{A}

\Phi = K \phi

Here,

\Phi

represents the flux linkage through a connected search coil, ensuring the deflection remains independent of the rate of flux change, provided it occurs over a duration of up to several seconds. The construction emphasizes this by employing a massive moving coil with very high moment of inertia, suspended via flexible ligaments rather than a traditional torsional fiber. This setup, often incorporating electromagnetic damping and a permanent magnet field, minimizes external influences and supports the coil's rotation in response to induced currents.^[42]^[43] The primary advantages of the Grassot fluxmeter lie in its insensitivity to circuit resistance (effective up to about 8 ohms) and the duration of flux variations, allowing accurate measurements of transient or varying magnetic fields without the damping or timing corrections required in other ballistic devices.^[44] It is particularly valued for determining the ballistic coefficient in magnetic studies, where the final deflection provides a direct measure of total flux impulse. In practice, it has been employed for transformer testing, such as evaluating core losses and hysteresis loops, and for characterizing magnetic materials through B-H curve determinations. Despite the advent of digital alternatives, the Grassot fluxmeter continues to be used in specialized laboratory settings into the 21st century for its reliability in high-precision analog flux integration.^[42]^[44]

Info Pages

Talk Pages

Special Pages

Ballistic galvanometer

Recent from talks

Recent from talks

Contribute something

Contribute something

Media Pages

Timelines

Articles

Notes collections

Notes

Notes

Days in Chronicle

Ballistic galvanometer

Grassot Fluxmeter

References