GRADE 11 PRACTICE
Physics Problems: Magnetism, Grade 11
Magnetic field forces and induction.
Here the conditions and analysis of the solution can be read without an account. In the simulator, you need to collect the same analyzes yourself: “Given,” formulas, order of steps and answer.
Problem statements
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Problem #1
Magnetism: magnetic field forcesTo a current-carrying conductor 5\,\text{А} and length 40\,\text{см} maximum force acting in a magnetic field 5\,\text{мН}. What is the magnetic field induction?
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- I
- 5\,\text{А}
- \ell
- 40\,\text{см}=0{,}4\,\text{м}
- F_{\text{м}}
- 5\,\text{мН}=5\cdot 10^{-3}\,\text{Н}
B - ?
- F_{\text{м}} = I\ell B\sin\alpha
The force is maximum at an angle of 90°, so the sine is equal to one.
- B = \dfrac{F_{\text{м}}}{I\ell}B = \dfrac{5\cdot 10^{-3}\,\text{Н}}{5\,\text{А}\cdot 0{,}4\,\text{м}}B = 2{,}5\cdot 10^{-3}\,\text{Тл} = 2{,}5\,\text{мТл}
AnswerB = 2{,}5\cdot 10^{-3}\,\text{Тл}
Problem #2
Magnetism: magnetic field forcesWhat should be the angle between the conductor length 20\,\text{см} and the magnetic induction vector B=4\,\text{мТл}, so that with current 15\,\text{А} the strength was: a) 6\,\text{мН}, b) 18\,\text{мН}? Consider angles from 0° to 90°.
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- \ell
- 20\,\text{см}=0{,}2\,\text{м}
- B
- 4\,\text{мТл}=4\cdot 10^{-3}\,\text{Тл}
- I
- 15\,\text{А}
- F_1
- 6\cdot 10^{-3}\,\text{Н}
- F_2
- 18\cdot 10^{-3}\,\text{Н}
\alpha_1 - ?\alpha_2 - ?
- F = I\ell B\sin\alpha\ \Rightarrow\ \sin\alpha = \dfrac{F}{I\ell B}
- \sin\alpha_1 = \dfrac{6\cdot 10^{-3}}{15\cdot 0{,}2\cdot 4\cdot 10^{-3}}\alpha_1 = 0{,}5\ \Rightarrow\ \alpha_1 = 30^{\circ}
- \sin\alpha_2 = \dfrac{18\cdot 10^{-3}}{15\cdot 0{,}2\cdot 4\cdot 10^{-3}}1{,}5 > 1
Sine cannot be greater than one: the maximum force under these conditions is 12 mN, so 18 mN is unattainable.
Answer\alpha_1 = 30^{\circ}\alpha_2\ \text{не существует}
Problem #3
Magnetism: magnetic field forcesThe electron moves at a speed 2\cdot10^{7}\,\text{м/с} perpendicular to the field with induction 40\,\text{мТл}. Determine the Lorentz force, the radius of the trajectory and the period of revolution.
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- B
- 40\,\text{мТл}=40\cdot 10^{-3}\,\text{Тл}
- v
- 2\cdot 10^{7}\,\text{м/с}
- q
- 1{,}6\cdot 10^{-19}\,\text{Кл}
- m
- 9{,}1\cdot 10^{-31}\,\text{кг}
- \alpha
- 90^{\circ}
F_{\text{Л}} - ?R - ?T - ?
- F_{\text{Л}} = qvB\sin\alphaF_{\text{Л}} = 1{,}6\cdot 10^{-19}\cdot 2\cdot 10^{7}\cdot 40\cdot 10^{-3}F_{\text{Л}} = 1{,}28\cdot 10^{-13}\,\text{Н}
- F_{\text{Л}} = \dfrac{mv^{2}}{R}\ \Rightarrow\ R = \dfrac{mv^{2}}{F_{\text{Л}}}R = \dfrac{9{,}1\cdot 10^{-31}\cdot\left(2\cdot 10^{7}\right)^{2}}{1{,}28\cdot 10^{-13}}R = 0{,}0028\,\text{м} = 2{,}8\,\text{мм}
The Lorentz force plays the role of a centripetal force.
- T = \dfrac{2\pi R}{v}T = \dfrac{2\cdot 3{,}14\cdot 0{,}0028}{2\cdot 10^{7}}T = 8{,}9\cdot 10^{-10}\,\text{с}
AnswerF_{\text{Л}} = 1{,}28\cdot 10^{-13}\,\text{Н}R = 0{,}0028\,\text{м}T = 8{,}9\cdot 10^{-10}\,\text{с}
Problem #4
Magnetism: magnetic field forcesHomogeneous electric and magnetic fields are mutually perpendicular: E=0{,}5\,\text{кВ/м}, B=0{,}001\,\text{Тл}. The electron moves perpendicular to both fields. Find its speed and direction for uniform linear motion.
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- E
- 0{,}5\,\tfrac{\text{кВ}}{\text{м}}=500\,\tfrac{\text{В}}{\text{м}}
- B
- 0{,}001\,\text{Тл}
v - ?
- F_{\text{Л}} = F_{\text{э}}
The movement is uniform when the Lorentz force balances the electric force; We neglect the gravity force of the electron.
- qvB = qE\ \Rightarrow\ v = \dfrac{E}{B}v = \dfrac{500}{0{,}001}v = 5\cdot 10^{5}\,\tfrac{\text{м}}{\text{с}}
Force equilibrium condition: E + v × B = 0. When v is perpendicular to both fields, the direction of velocity coincides with E × B.
Answerv=5\cdot10^{5}\,\text{м/с},\quad\vec v\parallel\vec E\times\vec B
Problem #5
Magnetism: magnetic field forcesA proton flew into a magnetic field at a speed 500\,\text{км/с} perpendicular to the induction vector. Determine the orbital radius and orbital period at B=30\,\text{мТл}.
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- v
- 500\,\tfrac{\text{км}}{\text{с}}=500\cdot 10^{3}\,\text{м/с}
- \alpha
- 90^{\circ}
- B
- 30\cdot 10^{-3}\,\text{Тл}
- q
- 1{,}6\cdot 10^{-19}\,\text{Кл}
- m
- 1{,}67\cdot 10^{-27}\,\text{кг}
R - ?T - ?
- qvB = \dfrac{mv^{2}}{R}\ \Rightarrow\ R = \dfrac{mv}{qB}R = \dfrac{1{,}67\cdot 10^{-27}\cdot 500\cdot 10^{3}}{1{,}6\cdot 10^{-19}\cdot 30\cdot 10^{-3}}R = 0{,}174\,\text{м}
- T = \dfrac{2\pi R}{v} = \dfrac{2\pi m}{qB}T = \dfrac{2\cdot 3{,}14\cdot 0{,}174}{500\cdot 10^{3}}T = 2{,}2\cdot 10^{-6}\,\text{с}
The period does not depend on the particle speed.
AnswerR = 0{,}174\,\text{м}T = 2{,}2\cdot 10^{-6}\,\text{с}
Problem #6
Magnetism: magnetic field forcesIn a magnetic field with induction 4\,\text{мТл} a horizontal conductor of length 20\,\text{см} and mass 16\,\text{г}. The conductor is perpendicular to the induction vector. Determine the current.
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- B
- 4\cdot 10^{-3}\,\text{Тл}
- \ell
- 0{,}2\,\text{м}
- m
- 0{,}016\,\text{кг}
- \alpha
- 90^{\circ}
- g
- 10\,\tfrac{\text{м}}{\text{с}^{2}}
I - ?
- F_A = mg
Equilibrium: Ampere's force balances the force of gravity.
- I\ell B\sin\alpha = mg\ \Rightarrow\ I = \dfrac{mg}{\ell B\sin\alpha}I = \dfrac{0{,}016\cdot 10}{0{,}2\cdot 4\cdot 10^{-3}\cdot 1}I = 200\,\text{А}
AnswerI = 200\,\text{А}
Problem #7
Magnetism: electromagnetic inductionCoil diameter 5\,\text{см} has 200 turns and is in a magnetic field parallel to the axis of the coil. What is the EMF if 0{,}3\,\text{с} induction changed from 80\,\text{мТл} up to 20\,\text{мТл}?
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- d
- 5\,\text{см}=0{,}05\,\text{м}
- n
- 200
- \Delta t
- 0{,}3\,\text{с}
- B_1
- 80\cdot 10^{-3}\,\text{Тл}
- B_2
- 20\cdot 10^{-3}\,\text{Тл}
\varepsilon_i - ?
- S = \dfrac{\pi d^{2}}{4}S = \dfrac{3{,}14\cdot 0{,}05^{2}}{4}S = 0{,}002\,\text{м}^{2}
- \left|\Delta\Phi\right| = \left|B_2 - B_1\right|S
The field is parallel to the coil axis, so the cosine is equal to one.
- \varepsilon_i = \dfrac{n\left|\Delta\Phi\right|}{\Delta t}\varepsilon_i = \dfrac{200\cdot\left|20\cdot 10^{-3} - 80\cdot 10^{-3}\right|\cdot 0{,}002}{0{,}3}\varepsilon_i = 0{,}08\,\text{В}
Answer\varepsilon_i = 0{,}08\,\text{В}
Problem #8
Magnetism: electromagnetic inductionWhen the current in the coil changes by inductance 0{,}2\,\text{Гн} for 0{,}1\,\text{с} self-induced emf occurred 3\,\text{В}. How much has the current changed?
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- \Delta t
- 0{,}1\,\text{с}
- L
- 0{,}2\,\text{Гн}
- \varepsilon_{si}
- 3\,\text{В}
\Delta I - ?
- \varepsilon_{si} = \dfrac{L\left|\Delta I\right|}{\Delta t}\ \Rightarrow\ \left|\Delta I\right| = \dfrac{\varepsilon_{si}\,\Delta t}{L}\left|\Delta I\right| = \dfrac{3\cdot 0{,}1}{0{,}2}\Delta I = 1{,}5\,\text{А}
Answer\Delta I = 1{,}5\,\text{А}
Problem #9
Magnetism: electromagnetic inductionIn a coil with inductance 0{,}5\,\text{Гн} current flows 8\,\text{А}. What is the energy of the magnetic field? How to change the current so that the energy increases in 9 once?
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- L
- 0{,}5\,\text{Гн}
- I
- 8\,\text{А}
W_{\text{м}} - ?I' - ?
- W_{\text{м}} = \dfrac{LI^{2}}{2}W_{\text{м}} = \dfrac{0{,}5\cdot 8^{2}}{2}W_{\text{м}} = 16\,\text{Дж}
- W \sim I^{2}\ \Rightarrow\ I \sim \sqrt{W}I' = 3I = 24\,\text{А}
Energy grows as the square of the current, so to increase by 9 times the current must be tripled.
AnswerW_{\text{м}} = 16\,\text{Дж}I' = 24\,\text{А}
Problem #10
Magnetism: electromagnetic inductionClosed resistance conductor 3\,\text{Ом} is in a magnetic field. What charge will pass through the conductor when the magnetic flux changes by 3\cdot10^{-4}\,\text{Вб}?
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- R
- 3\,\text{Ом}
- \Delta\Phi
- 3\cdot 10^{-4}\,\text{Вб}
q - ?
- \varepsilon_i = \dfrac{\left|\Delta\Phi\right|}{\Delta t},\quad I = \dfrac{\varepsilon_i}{R}
The induction current is determined by Faraday's law and Ohm's law.
- q = I\,\Delta t = \dfrac{\left|\Delta\Phi\right|}{R}q = \dfrac{3\cdot 10^{-4}}{3}q = 1\cdot 10^{-4}\,\text{Кл}
Time is reduced: charge depends only on changes in flux and resistance.
Answerq = 1\cdot 10^{-4}\,\text{Кл}
Problem #11
Magnetism: magnetic field forcesAn electron flies perpendicularly into a magnetic field with a speed 5\,\text{Мм/с} and moves in a circle with radius 1{,}1\,\text{см}. Determine the field induction and revolution period.
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- \alpha
- 90^{\circ}
- v
- 5\,\tfrac{\text{Мм}}{\text{с}}=5\cdot 10^{6}\,\text{м/с}
- R
- 1{,}1\,\text{см}=1{,}1\cdot 10^{-2}\,\text{м}
- q
- 1{,}6\cdot 10^{-19}\,\text{Кл}
- m
- 9{,}1\cdot 10^{-31}\,\text{кг}
B - ?T - ?
- qvB = \dfrac{mv^{2}}{R}\ \Rightarrow\ B = \dfrac{mv}{qR}B = \dfrac{9{,}1\cdot 10^{-31}\cdot 5\cdot 10^{6}}{1{,}6\cdot 10^{-19}\cdot 1{,}1\cdot 10^{-2}}B = 2{,}6\cdot 10^{-3}\,\text{Тл}
- T = \dfrac{2\pi R}{v}T = \dfrac{2\cdot 3{,}14\cdot 1{,}1\cdot 10^{-2}}{5\cdot 10^{6}}T = 1{,}38\cdot 10^{-8}\,\text{с}
AnswerB = 2{,}6\cdot 10^{-3}\,\text{Тл}T = 1{,}38\cdot 10^{-8}\,\text{с}
Problem #92
Magnetic field and forcesConductor length 0{,}2 m with current 5 A is located perpendicular to the magnetic field 0{,}4 Tl. Find the Ampere force.
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- l
- 0{,}2\,\text{м}
- I
- 5\,\text{А}
- B
- 0{,}4\,\text{Тл}
F - ?
- F=BIlF=0{,}4 \cdot 5 \cdot 0{,}2F=0{,}4\,\text{Н}
The angle is 90°, the sine is equal to one.
Answer0{,}4\,\text{Н}
Problem #93
Magnetic field and forcesConductor length 0{,}4 m with current 3 A is located perpendicular to the magnetic field 0{,}5 Tl. Find the Ampere force.
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- l
- 0{,}4\,\text{м}
- I
- 3\,\text{А}
- B
- 0{,}5\,\text{Тл}
F - ?
- F=BIlF=0{,}5 \cdot 3 \cdot 0{,}4F=0{,}6\,\text{Н}
The angle is 90°, the sine is equal to one.
Answer0{,}6\,\text{Н}
Problem #94
Magnetic field and forcesHorizontal conductor with mass 20 g and length 0{,}2 m is in a perpendicular field 0{,}5 Tl. What current is needed for the upward force of Ampere to balance the gravity? g = 10 m/s².
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- m
- 20\,\text{г}
- l
- 0{,}2\,\text{м}
- B
- 0{,}5\,\text{Тл}
- g
- 10\,\text{м/с}^{2}
I - ?
- F=mgF=\frac{20}{1000} \cdot 10F=0{,}2\,\text{Н}
Convert the mass into kilograms and find the force of gravity.
- I=\frac{F}{Bl}I=\frac{0{,}2}{(0{,}5 \cdot 0{,}2)}I=2\,\text{А}
At equilibrium BIl = mg.
Answer2\,\text{А}
Problem #95
Magnetic field and forcesHorizontal conductor with mass 30 g and length 0{,}3 m is in a perpendicular field 0{,}5 Tl. What current is needed for the upward force of Ampere to balance the gravity? g = 10 m/s².
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- m
- 30\,\text{г}
- l
- 0{,}3\,\text{м}
- B
- 0{,}5\,\text{Тл}
- g
- 10\,\text{м/с}^{2}
I - ?
- F=mgF=\frac{30}{1000} \cdot 10F=0{,}3\,\text{Н}
Convert the mass into kilograms and find the force of gravity.
- I=\frac{F}{Bl}I=\frac{0{,}3}{(0{,}5 \cdot 0{,}3)}I=2\,\text{А}
At equilibrium BIl = mg.
Answer2\,\text{А}
Problem #96
Magnetic field and forcesParticle with charge 0{,}000001 Cl and mass 1\cdot 10^{-9} kg moves perpendicular to the field 0{,}2 Tl with speed 100 m/s. Find the radius of the circle.
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- q
- 0{,}000001\,\text{Кл}
- m
- 1\cdot 10^{-9}\,\text{кг}
- B
- 0{,}2\,\text{Тл}
- v
- 100\,\text{м/с}
r - ?
- F=|q|vBF=0{,}000001 \cdot 100 \cdot 0{,}2F=0{,}00002\,\text{Н}
Magnetic force is perpendicular to speed.
- a=\frac{F}{m}a=\frac{0{,}00002}{1\cdot 10^{-9}}a=20000\,\text{м/с}^{2}
This is centripetal acceleration.
- r=\frac{v^2}{a}r=\frac{{100}^{2}}{20000}r=0{,}5\,\text{м}
We obtain the radius from a = v²/r.
Answer0{,}5\,\text{м}
Problem #97
Magnetic field and forcesParticle with charge 0{,}000002 Cl and mass 2\cdot 10^{-9} kg moves perpendicular to the field 0{,}4 Tl with speed 200 m/s. Find the radius of the circle.
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- q
- 0{,}000002\,\text{Кл}
- m
- 2\cdot 10^{-9}\,\text{кг}
- B
- 0{,}4\,\text{Тл}
- v
- 200\,\text{м/с}
r - ?
- F=|q|vBF=0{,}000002 \cdot 200 \cdot 0{,}4F=0{,}00016\,\text{Н}
Magnetic force is perpendicular to speed.
- a=\frac{F}{m}a=\frac{0{,}00016}{2\cdot 10^{-9}}a=80000\,\text{м/с}^{2}
This is centripetal acceleration.
- r=\frac{v^2}{a}r=\frac{{200}^{2}}{80000}r=0{,}5\,\text{м}
We obtain the radius from a = v²/r.
Answer0{,}5\,\text{м}
Problem #98
Magnetic flux and inductionUniform magnetic field 0{,}2 T perpendicular to the plane of the frame with area 0{,}04 m². Find the magnetic flux.
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- B
- 0{,}2\,\text{Тл}
- S
- 0{,}04\,\text{м}^{2}
\Phi - ?
- \Phi=BS\Phi=0{,}2 \cdot 0{,}04\Phi=0{,}008\,\text{Вб}
The normal to the frame is parallel to the field.
Answer0{,}008\,\text{Вб}
Problem #99
Magnetic flux and inductionUniform magnetic field 0{,}3 T perpendicular to the plane of the frame with area 0{,}06 m². Find the magnetic flux.
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- B
- 0{,}3\,\text{Тл}
- S
- 0{,}06\,\text{м}^{2}
\Phi - ?
- \Phi=BS\Phi=0{,}3 \cdot 0{,}06\Phi=0{,}018\,\text{Вб}
The normal to the frame is parallel to the field.
Answer0{,}018\,\text{Вб}
Problem #100
Magnetic flux and inductionThe flux through each turn of the coil is from 100 turns decreased uniformly from 0{,}006 Wb to zero for 0{,}2 s. Find the module of the induced emf.
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- N
- 100\,\text{витков}
- F
- 0{,}006\,\text{Вб}
- t
- 0{,}2\,\text{с}
|\mathcal{E}| - ?
- a=\frac{|\Delta\Phi|}{\Delta t}a=\frac{0{,}006}{0{,}2}a=0{,}03\,\text{Вб/с}
Find the rate of change of flow after one turn.
- |\mathcal{E}|=Na|\mathcal{E}|=100 \cdot 0{,}03|\mathcal{E}|=3\,\text{В}
The EMF of the turns adds up.
Answer3\,\text{В}
Problem #101
Magnetic flux and inductionThe flux through each turn of the coil is from 200 turns decreased uniformly from 0{,}004 Wb to zero for 0{,}4 s. Find the module of the induced emf.
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- N
- 200\,\text{витков}
- F
- 0{,}004\,\text{Вб}
- t
- 0{,}4\,\text{с}
|\mathcal{E}| - ?
- a=\frac{|\Delta\Phi|}{\Delta t}a=\frac{0{,}004}{0{,}4}a=0{,}01\,\text{Вб/с}
Find the rate of change of flow after one turn.
- |\mathcal{E}|=Na|\mathcal{E}|=200 \cdot 0{,}01|\mathcal{E}|=2\,\text{В}
The EMF of the turns adds up.
Answer2\,\text{В}
Problem #102
Magnetic flux and inductionA field perpendicular to a frame with an area 0{,}1 m², decreases evenly with 0{,}8 up to 0{,}2 Tl for 0{,}2 s. Frame resistance 3 Ohm. Find the magnitude of the induction current, neglect self-induction.
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- S
- 0{,}1\,\text{м}^{2}
- B_1
- 0{,}8\,\text{Тл}
- B_2
- 0{,}2\,\text{Тл}
- t
- 0{,}2\,\text{с}
- R
- 3\,\text{Ом}
I - ?
- |\Delta\Phi|=(B_1-B_2)S|\Delta\Phi|=(0{,}8 - 0{,}2) \cdot 0{,}1|\Delta\Phi|=0{,}06\,\text{Вб}
The frame area does not change.
- |\mathcal{E}|=\frac{|\Delta\Phi|}{t}|\mathcal{E}|=\frac{0{,}06}{0{,}2}|\mathcal{E}|=0{,}3\,\text{В}
We use the law of induction.
- I=\frac{|\mathcal{E}|}{R}I=\frac{0{,}3}{3}I=0{,}1\,\text{А}
The current module is determined by Ohm's law.
Answer0{,}1\,\text{А}
Problem #103
Magnetic flux and inductionA field perpendicular to a frame with an area 0{,}2 m², decreases evenly with 0{,}9 up to 0{,}3 Tl for 0{,}3 s. Frame resistance 4 Ohm. Find the magnitude of the induction current, neglect self-induction.
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- S
- 0{,}2\,\text{м}^{2}
- B_1
- 0{,}9\,\text{Тл}
- B_2
- 0{,}3\,\text{Тл}
- t
- 0{,}3\,\text{с}
- R
- 4\,\text{Ом}
I - ?
- |\Delta\Phi|=(B_1-B_2)S|\Delta\Phi|=(0{,}9 - 0{,}3) \cdot 0{,}2|\Delta\Phi|=0{,}12\,\text{Вб}
The frame area does not change.
- |\mathcal{E}|=\frac{|\Delta\Phi|}{t}|\mathcal{E}|=\frac{0{,}12}{0{,}3}|\mathcal{E}|=0{,}4\,\text{В}
We use the law of induction.
- I=\frac{|\mathcal{E}|}{R}I=\frac{0{,}4}{4}I=0{,}1\,\text{А}
The current module is determined by Ohm's law.
Answer0{,}1\,\text{А}
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