gyroradius造句

例句与造句

1. The radius of this motion is the gyroradius.
2. The radius of the circle that the particle describes is called the radius of gyration or gyroradius.
3. Their gyroradius shrinks and when they hit a dense magnetic field they can be reflected using the magnetic mirror effect.
4. Because particles passed through locations with no magnetic field, their motions could be straight, with an infinite gyroradius.
5. Inside the MaGrid, single electrons travel straight through the null point, due to their infinite gyroradius in regions of no magnetic field.
6. It's difficult to find gyroradius in a sentence. 用gyroradius造句挺难的
7. However, the gyroradius in those circumstances is also larger, so that the radial component of the magnetic field seen by the particle is also larger.
8. The size of this region is related to the s-parameter, or the ratio of the distance between the null and separatrix, and the thermal ion gyroradius.
9. To be able to proceed we set V = R \ omega _ g, where \ omega _ g = qB / m is the gyro frequency and is the gyroradius.
10. *The large diameter is more to do with the Gyroradius of a high energy charged particle than some difficulty in accelerating them . talk ) 09 : 13, 20 September 2009 ( UTC)
11. The radial magnetic field is designed to be strong enough to substantially deflect the low-mass electrons, but not the high-mass ions, which have a much larger gyroradius and are hardly impeded.
12. In a uniform magnetic field, a particle undergoes random walk across the field lines by the step size of gyroradius ?a " v th / ?, where v th denotes the thermal velocity, and ?a " qB / mc, the gyrofrequency.
13. If one assumed that magnetopause was just a boundary between a magnetic field in a vacuum and a plasma with a weak magnetic field embedded in it, then the magnetopause would be defined by electrons and ions penetrating one gyroradius into the magnetic field domain.
14. In a magnetized plasma, the collision frequency is usually small compared to the gyrofrequency, so that the step size is the gyroradius \ rho and the step time is the collision time, \ tau, which is related to the collision frequency through \ tau = 1 / \ nu, leading to D = \ rho ^ 2 \ nu.
15. The first and third terms to the Hasegawa Mima equation, which are the same as the Navier Stokes equation, are the terms introduced by adding the polarization drift . In the limit where the wavelength of a perturbation of the electric potential is much smaller than the gyroradius based on the sound speed, the Hasegawa Mima equations become the same as the two-dimensional incompressible fluid.