lies Suppose a magnetic field B(t) oscillates with frequency w. A circular loop of copper perpendicular to the magnetic field. The radius of the circular loop is r. a. Write down an expression for the magnetic field as a function of time. Determine the induced emf & in the loop of wire and use this to calculate the current generated in the loop as a function of time. b. What is the power dissipation in the wire as a function to time? Make a sketch of this function. What is the average power Pave dissipation in the wire? Hint: what is the average value of the function you sketched? C. Recall that power is a rate of energy transfer, and that power dissipated by a resistor leads to a change in the thermal energy of the material (in this case the copper wire). We can relate a ΔΕth change in thermal energy to a change in temperature by AT where M is the total mass and c = Mc is the specific heat capacity of the material (see page 526 for details). Find an expression for a dT differential change in temperature of the copper wire loop. dt d. Suppose the copper is initially at some temperature To. Find an expression for the temperature of the loop as a function of the time T(t) it is exposed to the oscillating magnetic field. Hint: Integrate. e. Suppose that a 10.0 mT magnetic field oscillates at 1000 Hz, and the radius of the loop is 2.0 cm. Assuming the initial temperature was To = 283 K, calculate the temperature of the copper loop after 1.0 minute of exposure to the oscillating magnetic field. The mass density of copper is Pm = 8.96 g/cm³. The resistivity of copper is found in table 27.2 and the specific heat capacity is found on page 526. Express your answer in °C. Comment on the result. Is this a large change in temperature? Suggest a practical application for this technology. How could this be used?
lies Suppose a magnetic field B(t) oscillates with frequency w. A circular loop of copper perpendicular to the magnetic field. The radius of the circular loop is r. a. Write down an expression for the magnetic field as a function of time. Determine the induced emf & in the loop of wire and use this to calculate the current generated in the loop as a function of time. b. What is the power dissipation in the wire as a function to time? Make a sketch of this function. What is the average power Pave dissipation in the wire? Hint: what is the average value of the function you sketched? C. Recall that power is a rate of energy transfer, and that power dissipated by a resistor leads to a change in the thermal energy of the material (in this case the copper wire). We can relate a ΔΕth change in thermal energy to a change in temperature by AT where M is the total mass and c = Mc is the specific heat capacity of the material (see page 526 for details). Find an expression for a dT differential change in temperature of the copper wire loop. dt d. Suppose the copper is initially at some temperature To. Find an expression for the temperature of the loop as a function of the time T(t) it is exposed to the oscillating magnetic field. Hint: Integrate. e. Suppose that a 10.0 mT magnetic field oscillates at 1000 Hz, and the radius of the loop is 2.0 cm. Assuming the initial temperature was To = 283 K, calculate the temperature of the copper loop after 1.0 minute of exposure to the oscillating magnetic field. The mass density of copper is Pm = 8.96 g/cm³. The resistivity of copper is found in table 27.2 and the specific heat capacity is found on page 526. Express your answer in °C. Comment on the result. Is this a large change in temperature? Suggest a practical application for this technology. How could this be used?
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