Chapter 5: Problem 8
An aircraft is flying at \(800 \mathrm{~km} \mathrm{~h}^{-1}\) in latitude \(55^{\circ} \mathrm{N}\). Find the angle through which it must tilt its wings to compensate for the horizontal component of the Coriolis force.
Chapter 5: Problem 8
An aircraft is flying at \(800 \mathrm{~km} \mathrm{~h}^{-1}\) in latitude \(55^{\circ} \mathrm{N}\). Find the angle through which it must tilt its wings to compensate for the horizontal component of the Coriolis force.
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Get started for freeA beam of particles of charge \(q\) and velocity \(v\) is emitted from a point source, roughly parallel with a magnetic field \(\boldsymbol{B}\), but with a small angular dispersion. Show that the effect of the field is to focus the beam to a point at a distance \(z=2 \pi m v /|q| B\) from the source. Calculate the focal distance for electrons of kinetic energy \(500 \mathrm{eV}\) in a magnetic field of \(0.01 \mathrm{~T}\). (Charge on electron \(=-1.6 \times 10^{-19} \mathrm{C}\), mass \(=9.1 \times 10^{-31} \mathrm{~kg}\), \(\left.1 \mathrm{eV}=1.6 \times 10^{-19} \mathrm{~J} .\right)\)
Find the equation of motion for a particle in a uniformly accelerated frame, with acceleration \(\boldsymbol{a} .\) Show that for a particle moving in a uniform gravitational field, and subject to other forces, the gravitational field may be eliminated by a suitable choice of \(\boldsymbol{a}\).
Another way of deriving the equation of motion (5.16) is to use Lagrange's equations. Express the kinetic energy \(\frac{1}{2} m(\mathrm{~d} \boldsymbol{r} / \mathrm{d} t)^{2}\) in terms of \((x, y, z)\), and show that Lagrange's equations (3.44) reproduce (5.16) for the case where the force is conservative.
A projectile is launched due north from a point in colatitude \(\theta\) at an angle \(\pi / 4\) to the horizontal, and aimed at a target whose distance is \(y\) (small compared to Earth's radius \(R\) ). Show that if no allowance is made for the effects of the Coriolis force, the projectile will miss its target by a distance \(x=\omega\left(\frac{2 y^{3}}{g}\right)^{1 / 2}\left(\cos \theta-\frac{1}{3} \sin \theta\right)\) Evaluate this distance if \(\theta=45^{\circ}\) and \(y=40 \mathrm{~km}\). Why is it that the deviation is to the east near the north pole, but to the west both on the equator and near the south pole? (Neglect atmospheric resistance.)
Write down the equation of motion for a charged particle in uniform, parallel electric and magnetic fields, both in the \(z\)-direction, and solve it, given that the particle starts from the origin with velocity \((v, 0,0)\). A screen is placed at \(x=a\), where \(a \ll m v / q B .\) Show that the locus of points of arrival of particles with given \(m\) and \(q\), but different speeds \(v\), is approximately a parabola. How does this locus depend on \(m\) and \(q ?\)
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