Question Video: Determining the Speed of a Straight Conductor Moving in a Uniform Magnetic Field | Nagwa Question Video: Determining the Speed of a Straight Conductor Moving in a Uniform Magnetic Field | Nagwa

Question Video: Determining the Speed of a Straight Conductor Moving in a Uniform Magnetic Field Physics • Third Year of Secondary School

A conducting rod moves on conducting rails that form a circuit that contains two resistors, as shown in the diagram. The power dissipated by the circuit is 65.5 mW. The strength of the magnetic field the circuit is within is 945 mT. The rod has a resistance per unit length of 15 Ω/m. Find the speed 𝑣 at which the rod must move.

04:43

Video Transcript

A conducting rod moves on conducting rails that form a circuit that contains two resistors, as shown in the diagram. The power dissipated by the circuit is 65.5 milliwatts. The strength of the magnetic field the circuit is within is 945 milliteslas. The rod has a resistance per unit length of 15 ohms per meter. Find the speed 𝑣 at which the rod must move.

Let’s start by taking a closer look at this circuit. We see two resistors with known resistance values. So let’s label them as 𝑅 one and 𝑅 two. But this circuit actually consists of three resistors, because the rod also has some resistance whose value we don’t currently know but we will be able to calculate. For now, let’s just call the resistance of the rod 𝑅 sub 𝑟. Notice that there’s no symbol showing a cell in this circuit, and that’s okay.

Recall that when a straight conducting rod moves through a uniform magnetic field, an electromotive force, or emf, is induced across the rod with a magnitude of 𝑙𝑣𝐵 sin 𝜃, where 𝑙 is the length of the rod, 𝑣 is the speed of the rod, 𝐵 is the strength of the magnetic field, and 𝜃 is the angle between the rod’s velocity and the magnetic field.

In this question, the rod is moving to the right and the magnetic field points out of the screen. So the rod’s velocity is perpendicular to the magnetic field, and 𝜃 equals 90 degrees. We know that the sin of 90 degrees simply equals one, which means that an emf of magnitude 𝑙𝑣𝐵 will be induced across the rod as it moves. In this way, the moving rod functions as a cell. So this will be the source of potential difference for the circuit.

Now, this question is asking us to solve for 𝑣, the speed of the rod. So let’s rearrange this formula to make 𝑣 the subject. To do this, we just need to divide both sides by 𝑙𝐵 so those terms cancel out, leaving 𝑣 by itself on one side of the equal sign. Thus, we have that 𝑣 equals the induced emf divided by 𝑙𝐵.

We already know that 𝑙 equals 25 centimeters, or 0.25 meters, and that the strength of the magnetic field 𝐵 equals 945 milliteslas, or 0.945 teslas. We don’t know the magnitude of the induced emf. So we need to find a way to express it in terms of values that we do know. Notice that we were given the power dissipated by the circuit, 𝑃, which equals 65.5 milliwatts, or 0.0655 watts. We can relate this power to emf using the formula power equals the emf squared divided by 𝑅. And we can easily solve this equation for the emf by multiplying both sides by 𝑅 and then taking the square root of both sides. Thus, emf equals the square root of 𝑃 times 𝑅.

Now, we can substitute this expression for the emf into the formula for speed. So it becomes 𝑣 equals the square root of 𝑃𝑅 divided by 𝑙𝐵. We’re getting closer. We already know 𝑃, 𝑙, and 𝐵, but we don’t yet know 𝑅, the total resistance of the circuit. So we’ll need to calculate it. Let’s refer to this value as 𝑅 total from now on.

To calculate the total resistance, let’s note that the resistors 𝑅 one and 𝑅 two are connected in parallel to the potential difference source and that the resistance of the rod can be modeled as a resistor 𝑅 sub 𝑟 that’s connected in series with the potential difference source. Thus, to find the total resistance of the circuit, we’ll first find the equivalent resistance of 𝑅 one and 𝑅 two. So let’s recall the formula for combining two resistors in parallel.

Substituting in those two resistance values, we have that their equivalent resistance equals 11.52 ohms. Thus, the circuit’s total resistance equals this value plus the resistance of the rod. We were told that the rod has a resistance per unit length of 15 ohms per meter. And since the rod is 0.25 meters long, we know that it has a resistance of 3.75 ohms. Therefore, the total resistance of the circuit equals 11.52 ohms plus 3.75 ohms, or 15.27 ohms.

Finally, we’re ready to calculate the speed of the rod 𝑣. Substituting in values for all the terms on the right-hand side, we know that since they’re all expressed in their appropriate base SI or SI-derived units, the units will work out nicely to give us a speed expressed in meters per second. Now, grabbing a calculator, we get a result of about 4.233 meters per second. And choosing to round this to one decimal place, we have our final answer. We’ve found that the rod must be moving through the magnetic field at a speed of 4.2 meters per second.

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