A charged particle is projected through a region in a gravity-free space. If it passes through the region with constant speed, then the region may have:
1. \(\vec{E}=0, \vec{B} \neq 0\)
2. \(\vec{E} \neq 0, \vec{B} \neq 0\)
3. \(\vec{E} \neq 0, \vec{B}=0\)
4. Both (1) & (2)
Which of the following statements about cyclotron is correct?
1. | A charged particle accelerates only between the dees because of the magnetic field. |
2. | A charged particle accelerates only between the dees because of the electric field. |
3. | A charged particle slows down within the dees and speeds up between the dees. |
4. | A charged particle continuously accelerates all the time. |
A neutron, a proton, an electron and an \(\alpha\text-\)particle enter a region of the uniform magnetic field with the same velocity. The magnetic field is perpendicular and directed into the plane of the paper. The tracks of the particles are labelled in the figure.
Which track will the \(\alpha\text-\)particle follow?
1. | \(A\) | 2. | \(B\) |
3. | \(C\) | 4. | \(D\) |
Suppose a cyclotron is operated at an oscillator frequency of 12 MHz and a discharge radius of 53 cm. What is the resulting kinetic energy of the deuterons?
(Mass of deuteron, \(m=3.34\times10^{-27}\) kg)
1. 16.6 MeV
2. 12 MeV
3. 15 MeV
4. 14 MeV
What is the primary function of the electric field in a cyclotron?
1. energize the charged particle.
2. bring the charged particle again and again into the field.
3. cancel the force due to the magnetic field.
4. guide charged particles to the exit part.
Which one of the following expressions represents Biot-Savart's law? Symbols have their usual meanings.
1. | \(\overrightarrow{d B}=\frac{\mu_0 \mathrm{I}(\overrightarrow{d l} \times \hat r)}{4 \pi|\overrightarrow{\mathrm{r}}|^3}\\ \) | 2. | \(\overrightarrow{d B}=\frac{\mu_0 \mathrm{I}(\overrightarrow{d l} \times \hat r)}{4 \pi|\overrightarrow{\mathrm{r}}|^2} \) |
3. | \(\overrightarrow{d B}=\frac{\mu_0 \mathrm{I}(\overrightarrow{d l} \times \vec{r})}{4 \pi|\vec{r}|^3} \) | 4. | \(\overrightarrow{d B}=\frac{\mu_0 \mathrm{I}(\overrightarrow{d l} \cdot \vec{r})}{4 \pi|\overrightarrow{\mathrm{r}}|^3}\) |
1. | \(\frac{120}{3}~\Omega \) | 2. | \(\frac{30}{7}~\Omega \) |
3. | \(\frac{170}{3}~\Omega \) | 4. | \(\frac{150}{7}~\Omega \) |
1. | \(B \over 2\) | 2. | \(2B\) |
3. | \(B \over 4\) | 4. | \(2B \over 3\) |
If a long hollow copper pipe carries a direct current along its length, then the magnetic field associated with the current will be:
1. | Only inside the pipe | 2. | Only outside the pipe |
3. | Both inside and outside the pipe | 4. | Zero everywhere |
1. \(\mu_{0} i_{1} i_{2}\)
2. \(\frac{\mu_{0} i_{1} i_{2}}{\pi}\)
3. \(\frac{\mu_{0} i_{1} i_{2}}{2 \pi}\)
4. \(2 \mu_{0} i_{1} i_{2}\)