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Calculate the magnetic field strength needed on a 200-turn square loop \(20.0 \mathrm{~cm}\) on a side to create a maximum torque of \(300 \mathrm{~N} \cdot \mathrm{m}\) if the loop is carrying \(25.0 \mathrm{~A}\).

Short Answer

Expert verified
Magnetic field strength needed is 1.5 T.

Step by step solution

01

Identify the known values

We have a 200-turn square loop with sides measuring \(20.0\,\mathrm{cm}\), carrying a current of \(25.0\,\mathrm{A}\), and needing to generate a maximum torque of \(300\,\mathrm{N}\cdot\mathrm{m}\).
02

Convert the side length to meters

Convert the side length from centimeters to meters: \(20.0\,\mathrm{cm} = 0.20\,\mathrm{m}\).
03

Calculate the area of the loop

The area \(A\) of a square is given by the formula \(A = \text{side}^2\). Substituting the side length gives \(A = (0.20)^2 = 0.04\,\mathrm{m}^2\).
04

Use the torque formula

The torque \(\tau\) on a coil in a magnetic field is given by \(\tau = nIAB \sin \theta\), where \(n\) is the number of turns, \(I\) is the current, \(A\) is the area, \(B\) is the magnetic field strength, and \(\theta\) is the angle between the normal to the coil and the magnetic field. For maximum torque, \(\sin \theta = 1\), therefore, \(\tau = nIAB\).
05

Solve for the magnetic field strength \(B\)

Rearrange the formula to solve for \(B\): \[ B = \frac{\tau}{nIA} \] Substituting the values: \[ B = \frac{300}{200 \times 25 \times 0.04} = \frac{300}{200} = 1.5\,\mathrm{T} \]
06

Answer verification step

Recalculate to ensure everything checks out:\[ B = \frac{300}{200 \times 25 \times 0.04} = \frac{300}{200} = 1.5\,\mathrm{T} \] The calculation confirms that the magnetic field strength is \(1.5\,\mathrm{T}\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Torque Calculation
Torque is a measure of how much a force acting on an object causes that object to rotate. It's fundamental in understanding rotational motion. In our scenario, torque is generated in a coil placed in a magnetic field. The formula for torque (\(\tau\)) in this context is:
  • \(\tau = n\times I \times A \times B \times \sin \theta\)
where:
  • \(n\) represents the number of turns in the coil,
  • \(I\) is the current flowing through the coil,
  • \(A\) is the area of the coil,
  • \(B\) is the magnetic field strength, and
  • \(\theta\) is the angle between the magnetic field and the normal to the plane of the coil.
For maximum torque, \(\sin \theta = 1\) as the field is perpendicular to the coil, simplifying our equation to \(\tau = n \times I \times A \times B\). By rearranging, you can solve for any variable if the others are known.
Square Loop
A square loop is simply a loop of wire where each side has equal length. In electromagnetism, square loops are frequently used in theoretical problems because they have straightforward geometric properties. Each side of our square loop is \(20.0\,\mathrm{cm}\), which is \(0.20\,\mathrm{m}\) when converted to meters.
The area \(A\) of the square loop is calculated as the side length squared, \(A = \text{side}^2\). For a square loop with a side of \(0.20\,\mathrm{m}\), the area will be \(0.20 \times 0.20 = 0.04\,\mathrm{m}^2\). This area quantitatively attributes to how the magnetic field interacts with the loop to produce torque.
Coil in Magnetic Field
When a coil or a loop of wire is placed in a magnetic field, it experiences a force that can cause it to rotate if the coil is carrying an electrical current. This is because magnetic fields exert a force on moving charges according to the right-hand rule.
The interaction between the magnetic field and the current generates torque, causing rotational motion. This principle is widely applied in electrical motors and generators where coils in magnetic fields convert electrical energy into mechanical motion, or vice versa. The critical point is the perpendicular interaction default for maximal torque, enhancing the efficiency of energy transfer.
Current in a Coil
Current refers to the flow of electric charge through a conductor, such as a coil. In our problem, the coil carries a current of \(25.0\,\mathrm{A}\). The presence of current in the wire creates a magnetic moment, which interacts with the external magnetic field.
The strength of the current, combined with the number of turns in the coil, significantly influences the torque produced.
  • The greater the current, or the more coils involved, the more considerable the torque generated, increasing the effectiveness of the coil as an actuator or motor component.
  • This principle highlights the importance of current magnitude in applications requiring significant force or motion.
Understanding the role of current in torque production is essential for designing electromagnetic devices.

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Most popular questions from this chapter

(a) Viewers of Star Trek hear of an antimatter drive on the Starship Enterprise. One possibility for such a futuristic energy source is to store antimatter charged particles in a vacuum chamber, circulating in a magnetic field, and then extract them as needed. Antimatter annihilates with normal matter, producing pure energy. What strength magnetic field is needed to hold antiprotons, moving at \(5.00 \times 10^{7} \mathrm{~m} / \mathrm{s}\) in a circular path \(2.00 \mathrm{~m}\) in radius? Antiprotons have the same mass as protons but the opposite (negative) charge. (b) Is this field strength obtainable with today's technology or is it a futuristic possibility?

How can the motion of a charged particle be used to distinguish between a magnetic and an electric field?

How far from the starter cable of a car, carrying \(150 \mathrm{~A}\), must you be to experience a field less than the Earth's \(\left(5.00 \times 10^{-5} \mathrm{~T}\right) ?\) Assume a long straight wire carries the current. (In practice, the body of your car shields the dashboard compass.)

An electron moving at \(4.00 \times 10^{3} \mathrm{~m} / \mathrm{s}\) in a 1.25-T magnetic field experiences a magnetic force of \(1.40 \times 10^{-16} \mathrm{~N}\). What angle does the velocity of the electron make with the magnetic field? There are two answers. (a) A physicist performing a sensitive measurement wants to limit the magnetic force on a moving charge in her equipment to less than \(1.00 \times 10^{-12} \mathrm{~N}\). What is the greatest the charge can be if it moves at a maximum speed of \(30.0 \mathrm{~m} / \mathrm{s}\) in the Earth's field? (b) Discuss whether it would be difficult to limit the charge to less than the value found in (a) by comparing it with typical static electricity and noting that static is often absent.

(a) A cosmic ray proton moving toward the Earth at \(5.00 \times 10^{7} \mathrm{~m} / \mathrm{s}\) experiences a magnetic force of \(1.70 \times 10^{-16} \mathrm{~N}\). What is the strength of the magnetic field if there is a \(45^{\circ}\) angle between it and the proton's velocity? (b) Is the value obtained in part (a) consistent with the known strength of the Earth's magnetic field on its surface? Discuss.

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