Vector treatment of the electric field

A test charge $q = 2\,\mu\text{C}$, placed at a point in a laboratory apparatus, experiences an electric force of $0.06\ \text{N}$. The situation is shown in the figure.

1. a) Calculate the electric field strength at that point, $E = \frac{F}{q}$, and state its SI unit.
2. b) Since the charge is positive, how are the direction and sense of $\vec{E}$ related to those of the force $\vec{F}$?

To measure the electric field at a point, a test charge is used.

1. a) Explain what a test charge is and why it should have a small value, so that it does not disturb the charges creating the field.
2. b) Write down the expression for the field created by a point charge $Q$ at a distance $r$ and reason, from it, why the field does not depend on the test charge used to measure it.

Draw in your notebook the electric field lines produced by a positive point charge and, separately, those of a negative point charge.

1. a) What does the direction of the arrows on the lines indicate? Relate it to the force that a positive test charge would experience.
2. b) Where is the field most intense, according to your drawing? Relate it to the expression $E = K \times \frac{Q}{r^2}$.

You can do it on paper and send a photo with your answer.

A small sphere charged with $Q = 5\,\mu\text{C}$ creates an electric field around it (take $K = 9\times10^{9}\ \text{N}\times\text{m}^2/\text{C}^2$). Look at the diagram:

1. a) Calculate the magnitude of the field at $0.3\ \text{m}$ from the sphere.
2. b) State the direction and sense of the field at that point, reasoning from the sign of the charge.

A space probe accumulates a net charge of $2\ \text{nC}$ due to bombardment by solar particles (take $K = 9\times10^{9}\ \text{N}\times\text{m}^2/\text{C}^2$). Assume the probe is approximately point-like.

1. a) Calculate the magnitude of the electric field it creates at $10\ \text{cm}$ from its surface (express the distance in metres).
2. b) Also calculate the field at $1\ \text{m}$ and check by what factor it has decreased when multiplying the distance by ten.

The field produced by a point charge is $E$ at a distance $r$.

1. a) Using the expression $E = K \times \frac{Q}{r^2}$, reason what value the field will have at a distance $2 \times r$ and at a distance $\frac{r}{3}$.
2. b) If the field at $0.5\ \text{m}$ from a certain charge is $7200\ \text{N/C}$, calculate its value at $1\ \text{m}$ without using the constant $K$.

A sensor measures an electric field of $4500\ \text{N/C}$ at $2\ \text{m}$ from the centre of a charged metal sphere in the laboratory; the field points towards the sphere (take $K = 9\times10^{9}\ \text{N}\times\text{m}^2/\text{C}^2$). The situation is represented in the figure.

1. a) Rearrange for charge in the expression $E = K \times \frac{Q}{r^2}$ and calculate its absolute value.
2. b) From the direction of the measured field, reason what the sign of the charge on the sphere is.

The manual of a medical diagnostic instrument requires that the electric field at its location must not exceed $500\ \text{N/C}$. Equipment that accumulates a point charge of $2\ \text{nC}$ operates in the same room (take $K = 9\times10^{9}\ \text{N}\times\text{m}^2/\text{C}^2$).

1. a) Rearrange for distance in the expression $E = K \times \frac{Q}{r^2}$ and calculate the minimum distance from the equipment at which the instrument must be installed.
2. b) If it is ultimately installed at twice that distance, by what factor is the field reduced? Reason your answer.

From the definition $E = \frac{F}{q}$, state which of these expressions are valid units for electric field strength and reason each answer:

1. a) $\text{N/C}$
2. b) $\text{N}\times\text{C}$
3. c) $\text{V/m}$ (note that $1\ \text{V} = 1\ \text{J/C}$)
4. d) $\text{J/C}$

Between the plates of a capacitor there is a uniform electric field $\vec{E} = 3\cdot10^{4}\,\vec{j}\ \text{N/C}$. A particle with charge $q = -4\,\mu\text{C}$ is placed inside it, as shown in the figure.

1. a) Calculate the electric force vector acting on the particle, $\vec{F} = q \cdot \vec{E}$, expressing it using the corresponding unit vector.
2. b) Reason why, since the charge is negative, the force is in the opposite direction to the field.

In a cathode ray tube, an electron passes through a region with a uniform electric field $E = 1000\ \text{N/C}$ (given: elementary charge $e = 1.6\times10^{-19}\ \text{C}$; mass of the electron $m_e = 9.11\times10^{-31}\ \text{kg}$).

1. a) Calculate the electric force on the electron.
2. b) Calculate its acceleration by applying Newton's second law, $a = \frac{F}{m_e}$.

A proton is between the plates of a capacitor, where the electric field is uniform and equal to $E = 2\times10^{4}\ \text{N/C}$ (given: elementary charge $e = 1.6\times10^{-19}\ \text{C}$; mass of the proton $m_p = 1.67\times10^{-27}\ \text{kg}$; take $g = 9.8\ \text{m/s}^2$).

1. a) Calculate the electric force on the proton.
2. b) Calculate its weight.
3. c) Calculate the ratio between both magnitudes and draw a conclusion: in particle physics, can gravity be neglected compared to the electric force?

A point charge $Q = 4\ \text{nC}$ is at the origin of coordinates (take $K = 9\times10^{9}\ \text{N}\times\text{m}^2/\text{C}^2$). Observe the diagram:

1. a) Calculate the magnitude of the electric field at the point $P(3, 4)$, with the coordinates in metres.
2. b) The radial unit vector at that point is $\vec{u}_r = \frac{3}{5}\,\vec{i} + \frac{4}{5}\,\vec{j}$. Write the vector $\vec{E}$ in terms of $\vec{i}$ and $\vec{j}$.

Two point charges $q_1 = 3\,\mu\text{C}$ and $q_2 = -2\,\mu\text{C}$ lie on the $x$-axis, at $x_1 = 0$ and $x_2 = 1\ \text{m}$ (take $K = 9\times10^{9}\ \text{N}\times\text{m}^2/\text{C}^2$). The figure shows the arrangement of the charges.

1. a) Calculate the field (magnitude and direction) produced by each charge at the point $x = 3\ \text{m}$.
2. b) Apply the superposition principle and calculate the total field at that point, stating its direction and sense.

Two identical charges $q = 5\ \text{nC}$ are separated by $40\ \text{cm}$ (take $K = 9\times10^{9}\ \text{N}\times\text{m}^2/\text{C}^2$).

1. a) By drawing the vectors in your notebook, reason what the value of the total field is at the midpoint of the line segment joining the charges.
2. b) Calculate the total field (magnitude, direction and sense) at a point on the segment situated at $10\ \text{cm}$ from one of the charges.

A charge $Q = 8\ \text{nC}$ is fixed to an insulating stand in the laboratory (take $K = 9\times10^{9}\ \text{N}\times\text{m}^2/\text{C}^2$).

1. a) Calculate the electric field (magnitude, direction and sense) at $25\ \text{cm}$ from the charge.
2. b) Calculate the force (magnitude, direction and sense) that a charge $q_0 = 3\,\mu\text{C}$ placed at that point would experience, using $\vec{F} = q_0 \cdot \vec{E}$.

Three identical charges $q = 2\ \text{nC}$ occupy the vertices of an equilateral triangle of side length $30\ \text{cm}$ (take $K = 9\times10^{9}\ \text{N}\times\text{m}^2/\text{C}^2$). Observe the diagram:

1. a) Justify, by symmetry (the three field vectors at the centre form angles of $120^\circ$ with each other), that the total field at the centre of the triangle is zero.
2. b) One of the charges is removed. Taking into account that the field of all three was zero, reason that the field of the remaining two is exactly the opposite of the one produced by the removed charge, and calculate its magnitude (the distance from each vertex to the centre is $\frac{0.3}{\sqrt{3}}\ \text{m}$).
3. c) State the direction and sense of the resultant field relative to the vertex that has been left empty.

Your classmate calculates the electric field at the midpoint of the segment joining a charge $q_1 = 6\,\mu\text{C}$ to another charge $q_2 = -6\,\mu\text{C}$, separated by $20\ \text{cm}$, and writes: "the field is zero, because the charges are opposite and cancel out" (take $K = 9\times10^{9}\ \text{N}\times\text{m}^2/\text{C}^2$).

1. a) Explain the error: draw the vectors $\vec{E}_1$ and $\vec{E}_2$ at the midpoint in your notebook and reason what sense each one has.
2. b) Calculate the correct field (magnitude, direction and sense) at that point.
3. c) For which pair of charges with the same absolute value would your classmate's result be correct? Justify your answer.

You can do it on paper and send a photo with your answer.

Two point charges $q_1 = 1\,\mu\text{C}$ and $q_2 = 4\,\mu\text{C}$ lie on the $x$-axis, at $x_1 = 0$ and $x_2 = 3\ \text{m}$ (take $K = 9\times10^{9}\ \text{N}\times\text{m}^2/\text{C}^2$). The figure shows the three regions of the axis.

1. a) Reason, by analysing the direction of the field from each charge, in which of the three regions of the axis (to the left of $q_1$, between the charges, or to the right of $q_2$) the total field can be zero.
2. b) Set up the condition for zero field in that region and calculate the exact point.
3. c) Check the result by verifying that at that point the two fields have the same magnitude.

In an inkjet printer, charged ink droplets are deflected by an electric field. To study the principle, consider an electron entering with horizontal velocity $v_0 = 3\times10^{7}\ \text{m/s}$ into a region of length $L = 10\ \text{cm}$ where there is a uniform vertical field $E = 10^{4}\ \text{N/C}$, perpendicular to its velocity (given: elementary charge $e = 1.6\times10^{-19}\ \text{C}$; mass of the electron $m_e = 9.11\times10^{-31}\ \text{kg}$). The diagram shows the setup.

1. a) Calculate the acceleration of the electron in the field region and state its direction and sense.
2. b) Calculate the time it takes to cross the region.
3. c) Assuming horizontal motion with constant velocity and vertical motion with constant acceleration (like in projectile motion), calculate the vertical deflection at the exit, $y = \frac{1}{2} \times a \times t^2$.
4. d) Reason what shape the trajectory has inside the field and what type of motion the electron executes after leaving it.

Two point charges $q_1 = q$ and $q_2 = -2 \times q$, with $q > 0$, lie on the $x$-axis, at $x_1 = 0$ and $x_2 = 3\ \text{m}$ (take $K = 9\times10^{9}\ \text{N}\times\text{m}^2/\text{C}^2$).

1. a) Predict, justifying it using the direction of the fields and the absolute values of the charges, in which region of the axis the total field can be zero: between the charges or outside the segment? And on which side?
2. b) Set up the zero-field equation and solve it, obtaining the exact point.
3. c) Explain why the result does not depend on the value of $q$.

In a chamber of a linear particle accelerator, there is a uniform vertical electric field $E = 5\times10^{3}\ \text{N/C}$. A proton and an electron enter it separately with the same horizontal velocity (given: elementary charge $e = 1.6\times10^{-19}\ \text{C}$; mass of the electron $m_e = 9.11\times10^{-31}\ \text{kg}$; mass of the proton $m_p = 1.67\times10^{-27}\ \text{kg}$).

1. a) Compare the magnitudes of the electric forces on both particles and reason why they are equal.
2. b) Calculate the acceleration of each particle.
3. c) Calculate the ratio $\frac{a_e}{a_p}$ and relate it to the mass ratio $\frac{m_p}{m_e}$.
4. d) Predict and justify: do both particles deflect to the same side? In the same time of flight, which one deflects more and by how many times?