Bundle: Physics for Scientists and Engineers with Modern Physics, Loose-leaf Version, 9th + WebAssign Printed Access Card, Multi-Term
Bundle: Physics for Scientists and Engineers with Modern Physics, Loose-leaf Version, 9th + WebAssign Printed Access Card, Multi-Term
9th Edition
ISBN: 9781305932302
Author: Raymond A. Serway, John W. Jewett
Publisher: Cengage Learning
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Chapter 29, Problem 44P

(a)

To determine

The magnetic force vector on ab.

(a)

Expert Solution
Check Mark

Answer to Problem 44P

The magnetic force vector on ab is 0N.

Explanation of Solution

Write the equation for the magnetic force vector on the conductor.

    FB=IL×B                                                                                                              (I)

Here, FB is the magnetic force vector, I is current, L is the length vector of the conductor and B is the magnetic field vector.

Conclusion:

Substitute 5.00A for I, 0.400j^m for L and 0.0200j^T for B in the equation (I) to calculate the magnetic force vector.

    FB=[(5.00A)(0.400j^m×0.0200j^T)]=(5.00A)[(0.400m)(0.0200T)(j^×j^)]=0N

Therefore, the magnetic force vector on ab is 0N.

(b)

To determine

The magnetic vector force on bc.

(b)

Expert Solution
Check Mark

Answer to Problem 44P

The magnetic force vector on bc is 0.040i^N.

Explanation of Solution

Conclusion:

Substitute 5.00A for I, 0.400k^m for L and 0.0200j^T for B in the equation (I) to calculate the magnetic force vector.

    FB=[(5.00A)(0.400k^m×0.0200j^T)]=(5.00A)[(0.400m)(0.0200T)(k^×j^)]=(5.00)[0.008i^]=0.040i^N

Therefore, the magnetic vector force on bc 0.040i^N.

(c)

To determine

The magnetic force vector on cd.

(c)

Expert Solution
Check Mark

Answer to Problem 44P

The magnetic force vector on cd is 0.040k^N.

Explanation of Solution

Conclusion:

Substitute 5.00A for I, (0.400i^m+0.400j^m) for L and 0.0200j^T for B in the equation (I) to calculate the magnetic force vector.

    FB=[(5.00A)[(0.400i^m+0.400j^m)×0.0200j^T]]=(5.00A)[(0.400m)(0.0200T)(i^×j^)+(0.400m)(0.0200T)(j^×j^)]=(5.00)[0.008k^+0]N=0.040k^N

Therefore, the magnetic force vector on cd is 0.040k^N.

(d)

To determine

The magnetic force vector on da.

(d)

Expert Solution
Check Mark

Answer to Problem 44P

The magnetic force vector on da is (0.040k^+0.040i^)N.

Explanation of Solution

Conclusion:

Substitute 5.00A for I, (0.400i^m0.400k^m) for L and 0.0200j^T for B in the equation (I) to calculate the magnetic force vector.

    FB=[(5.00A)[(0.400i^m0.400k^m)×0.0200j^T]]=(5.00A)[(0.400m)(0.0200T)(i^×j^)+(0.400m)(0.0200T)(k^×j^)]=(5.00)[0.008k^0.008i^]N=(0.040k^+0.040i^)N

Therefore, the magnetic force vector on da is (0.040k^+0.040i^)N.

(e)

To determine

The method to find the force exerted on the fourth segment due to the forces on the other three segments.

(e)

Expert Solution
Check Mark

Answer to Problem 44P

The force exerted on the fourth segment due to the forces on the other three segments is the negative of resultant of the sum of the forces on other three segments.

Explanation of Solution

The sum of the force on all the four segments is equal to zero. Hence, the force on the fourth vector will be equal to the negative of resultant of the sum of the forces on other three segments.

Conclusion:

Therefore, the force exerted on the fourth segment due to the forces on the other three segments is the negative of resultant of the sum of the forces on other three segments.

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Chapter 29 Solutions

Bundle: Physics for Scientists and Engineers with Modern Physics, Loose-leaf Version, 9th + WebAssign Printed Access Card, Multi-Term

Ch. 29 - Prob. 7OQCh. 29 - Prob. 8OQCh. 29 - Prob. 9OQCh. 29 - Prob. 10OQCh. 29 - Prob. 11OQCh. 29 - Prob. 12OQCh. 29 - Prob. 13OQCh. 29 - Prob. 1CQCh. 29 - Prob. 2CQCh. 29 - Prob. 3CQCh. 29 - Prob. 4CQCh. 29 - Prob. 5CQCh. 29 - Prob. 6CQCh. 29 - Prob. 7CQCh. 29 - At the equator, near the surface of the Earth, the...Ch. 29 - Prob. 2PCh. 29 - Prob. 3PCh. 29 - Consider an electron near the Earths equator. In...Ch. 29 - Prob. 5PCh. 29 - A proton moving at 4.00 106 m/s through a...Ch. 29 - Prob. 7PCh. 29 - Prob. 8PCh. 29 - A proton travels with a speed of 5.02 106 m/s in...Ch. 29 - Prob. 10PCh. 29 - Prob. 11PCh. 29 - Prob. 12PCh. 29 - Prob. 13PCh. 29 - An accelerating voltage of 2.50103 V is applied to...Ch. 29 - A proton (charge + e, mass mp), a deuteron (charge...Ch. 29 - Prob. 16PCh. 29 - Review. One electron collides elastically with a...Ch. 29 - Review. One electron collides elastically with a...Ch. 29 - Review. An electron moves in a circular path...Ch. 29 - Prob. 20PCh. 29 - Prob. 21PCh. 29 - Prob. 22PCh. 29 - Prob. 23PCh. 29 - A cyclotron designed to accelerate protons has a...Ch. 29 - Prob. 25PCh. 29 - Prob. 26PCh. 29 - A cyclotron (Fig. 28.16) designed to accelerate...Ch. 29 - Prob. 28PCh. 29 - Prob. 29PCh. 29 - Prob. 30PCh. 29 - Prob. 31PCh. 29 - Prob. 32PCh. 29 - Prob. 33PCh. 29 - Prob. 34PCh. 29 - A wire carries a steady current of 2.40 A. A...Ch. 29 - Prob. 36PCh. 29 - Prob. 37PCh. 29 - Prob. 38PCh. 29 - Prob. 39PCh. 29 - Consider the system pictured in Figure P28.26. A...Ch. 29 - Prob. 41PCh. 29 - Prob. 42PCh. 29 - Prob. 43PCh. 29 - Prob. 44PCh. 29 - Prob. 45PCh. 29 - A 50.0-turn circular coil of radius 5.00 cm can be...Ch. 29 - Prob. 47PCh. 29 - Prob. 48PCh. 29 - Prob. 49PCh. 29 - Prob. 50PCh. 29 - Prob. 51PCh. 29 - Prob. 52PCh. 29 - Prob. 53PCh. 29 - A Hall-effect probe operates with a 120-mA...Ch. 29 - Prob. 55PCh. 29 - Prob. 56APCh. 29 - Prob. 57APCh. 29 - Prob. 58APCh. 29 - Prob. 59APCh. 29 - Prob. 60APCh. 29 - Prob. 61APCh. 29 - Prob. 62APCh. 29 - Prob. 63APCh. 29 - Prob. 64APCh. 29 - Prob. 65APCh. 29 - Prob. 66APCh. 29 - A proton having an initial velocity of 20.0iMm/s...Ch. 29 - Prob. 68APCh. 29 - Prob. 69APCh. 29 - Prob. 70APCh. 29 - Prob. 71APCh. 29 - Prob. 72APCh. 29 - Prob. 73APCh. 29 - Prob. 74APCh. 29 - Prob. 75APCh. 29 - Prob. 76APCh. 29 - Prob. 77CPCh. 29 - Prob. 78CPCh. 29 - Review. A wire having a linear mass density of...Ch. 29 - Prob. 80CP
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