2019
DOI: 10.1109/tps.2018.2871563
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Modeling for the Calculation of Interior Ballistic Velocity of Electromagnetic Rail Launch Projectile

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Cited by 4 publications
(2 citation statements)
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“…where W is the inductive energy. Since the inductance during the launch process is not only related to the position of the ferromagnetic projectile x (t), but also related to the magnitude of the current i (t), the inductance is expressed as L(x,i ), the electromagnetic force on the projectile in the axial direction of the coil is: [13]…”
Section: Theoretical Analysis Of the Solving Methodsmentioning
confidence: 99%
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“…where W is the inductive energy. Since the inductance during the launch process is not only related to the position of the ferromagnetic projectile x (t), but also related to the magnitude of the current i (t), the inductance is expressed as L(x,i ), the electromagnetic force on the projectile in the axial direction of the coil is: [13]…”
Section: Theoretical Analysis Of the Solving Methodsmentioning
confidence: 99%
“… Wgoodbreak=12L(x,i)i2(t)$$ W=\frac{1}{2}L\left(x,i\right)\cdot {i}^2(t) $$ where W is the inductive energy. Since the inductance during the launch process is not only related to the position of the ferromagnetic projectile x ( t ), but also related to the magnitude of the current i ( t ), the inductance is expressed as L ( x,i ), the electromagnetic force on the projectile in the axial direction of the coil is: [13] Femgoodbreak=dWdxgoodbreak=12i2(t)L(x,i)x$$ {F}_{em}=\frac{dW}{dx}=\frac{1}{2}{i}^2(t)\cdot \frac{\partial L\left(x,i\right)}{\partial x} $$ …”
Section: Theoretical Analysis Of the Solving Methodsmentioning
confidence: 99%