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STRATEGIC INTERVENTION MATERIAL
AMPERE’S LAW
Prepared by:
Alvin P. Cajiles
Teacher I
Narra National High School
OBJECTIVE
Calculate magnetic fields for
highly symmetric current
configurations using
Ampere’s Law
(STEM12_GPEM-IIIi-65).
GUIDE CARD
Gauss’s Law allowed us to
find the net electric field
due to any charge
distribution by applying
symmetry.
Carl Friedrich
Gauss
Are we able to find the net
magnetic field due to
current if there is
symmetry? Let’s get help
from Ampere’s Law.
AndrΓ©-Marie
Ampère
GUIDE
CARD
Ampere’s Law is a
useful law that relates
the net magnetic field
along a closed loop to
the electric field current
passing through the
loop.
First discovered by
André-Marie Ampère in
GUIDE CARD
The integral around a closed path of the
component of the magnetic field tangent to the
direction of the path is equals to Β΅ times the
current I intercepted by the area within the
path.
𝐡. 𝑑𝑠 = πœ‡0 𝐼𝑒𝑛𝑐
GUIDE CARD
𝐡. 𝑑𝑠 = πœ‡0 𝐼𝑒𝑛𝑐
line integral
B.ds is integrated around
a closed loop called
Amperian Loop
Permeability
of free space
(constant)
Enclosed
current by the
curve
AMPERE’S LAW
GUIDE CARD
IMPORTANT NOTES
- All currents have to be steady and do not
change with time.
-Only currents crossing the area inside the path
are taken into account.
-Current have to be taken with their algebraic
sign by using the Right Hand Rule
GUIDE CARD
THE RIGHT HAND RULE for DETERMINING
THE DIRECTION OF MAGNETIC FIELD
ACTIVITY CARD No.1
Find the magnetic field outside a long straight
wire with current I and radius r.
I
r
Amperian
Loop
Wire surface
Direction of
Integration
Magnetic field
B
ds
r
cross-section of
the wire
ACTIVITY CARD No.2
What is the direction of magnetic field due to a
current passing through a solenoid?
Remember to use the
Right Hand Rule
where the thumb
takes the direction of
the current.
ACTIVITY CARD No.3
Use Ampere’s Law to
determine the
magnetic field
strength outside a
solenoid with n turns
(coils) per unit
length.
L
ASSESSMENT CARD No.1
Find the magnetic field inside a current-
carrying wire.
ds
r
R
R
I B
Amperian
Loop
ASSESSMENT CARD No.2
Calculate the magnetic field B in a
wire with radius 1Β΅m and the
current passing through it is 1 A.
Note that 𝝁 𝟎 = πŸ’π… 𝒙 πŸπŸŽβˆ’πŸ•
𝑻. π’Ž/𝑨.
ASSESSMENT CARD No.3
The magnetic field strength of a solenoid
is 0.0270T. Its radius is 0.40 m and length is
0.40 m. How many turns are there in the
solenoid if the steady current passing
through it is 12.0 A?
ENRICHMENT CARD
Magnetic Field of a
Toroid
The current enclosed by the dashed
line is just the number of loops times
the current in each loop. Ampere’s
Law then gives the magnetic field by
𝐡 2πœ‹π‘Ÿ = πœ‡0 𝑁𝐼
𝐡 =
πœ‡0 𝑁𝐼
2πœ‹π‘Ÿ
ENRICHMENT CARDToroid is a useful device used in many applications in telecommunication,
music instruments, medical field, ballasts, EMI filter among others to
direct and restrict magnetic fields.
ENRICHMENT CARD
Additional Helpful Reading
www.learnapphysics.com/apphysicsc/magnetism.php
AP Physics C – Ampere’s Law
https://www.youtube.com/watch?v=pLyrVDJ3qas&t=5s
REFERENCE CARD
AP Physics C – Amperes Law. (2013). Retrieved from https://www.youtube.com/watch?v=pLyrVDJ3qas&t=5s
Elert, G. (n.d.). Ampere’s Law – Problems – The Physics Hypertextbook. Retrieved from https://physics.info/law-
ampere/problems/shtml.
SS: Magnetic field due to current in a straight wire. (2015). Retrieved from https://www.miniphysics.com/ss-
magnetic-field-due-to-current-in-a-straight-wire.html
Solenoid. (n.d.). Retrieved from http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html
Toroidal Magnetic Field. (n.d.). Retrieved from http://hyperphysics.phyastr.gsu.edu/hbase/magnetic/toroid.html
White, R. (n.d.). Learn AP Physics – Magnetism. Retrieved from
http://www.learnapphysics.com/apphysicsc/magnetism.php
ACTIVITY No.1
𝐡. 𝑑𝑠 = πœ‡0 𝐼
𝐡 𝑑𝑠 = πœ‡0 𝐼
𝐡 2πœ‹π‘Ÿ = πœ‡0 𝐼
𝑑𝑠 = 2πœ‹π‘Ÿ β†’ π‘π‘–π‘Ÿπ‘π‘’π‘šπ‘“π‘’π‘Ÿπ‘’π‘›π‘π‘’ π‘œπ‘“ π‘Ž π‘π‘–π‘Ÿπ‘π‘™π‘’
𝐡 =
πœ‡0 𝐼
2πœ‹π‘Ÿ
ANSWER KEY
Activity No.2: Remember that Right Hand
Rule says that the thumb
takes the direction of the
current and the curl of the
palm is the direction of the
magnetic field. Thus, in this
case, the magnetic field is
like passing through the
solenoid.
ANSWER KEY
Activity No.3:
𝑩. 𝒅𝒔 = 𝝁 𝟎 𝑰
𝑩 𝒅𝒔 = 𝝁 𝟎 𝑰
𝒅𝒔 = 𝑳 β†’ 𝒕𝒐𝒕𝒂𝒍 π’π’†π’π’ˆπ’•π’‰ 𝒐𝒇 𝒕𝒉𝒆 π’˜π’Šπ’“π’†(π’”π’π’π’†π’π’π’Šπ’…)
𝑰 β†’ 𝒏𝑰 π’‚π’Žπ’π’–π’π’• 𝒐𝒇 𝒄𝒖𝒓𝒓𝒆𝒏𝒕 𝒅𝒖𝒆 𝒕𝒐 π’π’–π’Žπ’ƒπ’†π’“ 𝒐𝒇 𝒕𝒖𝒓𝒏𝒔
𝑩 𝑳 = 𝝁 𝟎 𝒏𝑰
∴ 𝑩 =
𝝁 𝟎 𝒏𝑰
𝑳
β†’ π’Žπ’‚π’ˆπ’π’†π’•π’Šπ’„ π’‡π’Šπ’†π’π’… π’Šπ’ 𝒂 π’”π’π’π’†π’π’π’Šπ’…
ANSWER KEY
Assessment No.1:
𝐡. 𝑑𝑠 = πœ‡0 𝐼
𝐡 𝑑𝑠 = πœ‡0 𝐼
𝐡 2πœ‹π‘Ÿ = πœ‡0 𝐼
𝑑𝑠 = 2πœ‹π‘Ÿ β†’ π‘π‘–π‘Ÿπ‘π‘’π‘šπ‘“π‘’π‘Ÿπ‘’π‘›π‘π‘’ π‘œπ‘“ π‘Ž π‘π‘–π‘Ÿπ‘π‘™π‘’
𝐼𝑒𝑛𝑐 =
πœ‹π‘Ÿ2 𝑖
πœ‹π‘…2 β†’charge enclosed is proportional to the area encircled by the loop
𝐡 (2πœ‹π‘Ÿ) = πœ‡0
πœ‹π‘Ÿ2 𝑖
πœ‹π‘…2
∴ 𝐡 =
πœ‡0 πΌπ‘Ÿ
2πœ‹π‘…2 β†’ π‘šπ‘Žπ‘”π‘›π‘’π‘‘π‘–π‘ 𝑓𝑖𝑒𝑙𝑑 𝑖𝑛 π‘Ž π‘π‘œπ‘Žπ‘₯π‘–π‘Žπ‘™ π‘π‘Žπ‘π‘™π‘’
ANSWER KEY
Assessment No.2:
𝐡 =
(4πœ‹ π‘₯ 10βˆ’7
𝑇. π‘š/𝐴)(1𝐴)
(2πœ‹)(1 π‘₯ 10βˆ’3 π‘š)
𝐡 = 200 πœ‡π‘‡
ANSWER KEY
Assessment No.3:
𝐡 =
πœ‡0 𝑁𝐼
𝐿
𝑁 =
𝐡𝐿
πœ‡0 𝐼
𝑁 =
𝐡𝐿
πœ‡0 𝐼
=
(0.0270 𝑇)(0.40 π‘š)
(4πœ‹ π‘₯ 10βˆ’7 𝑇.π‘š/𝐴)(12 𝐴)
= 716 π‘‘π‘’π‘Ÿπ‘›π‘ 
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Ampere's Law

  • 1. STRATEGIC INTERVENTION MATERIAL AMPERE’S LAW Prepared by: Alvin P. Cajiles Teacher I Narra National High School
  • 2. OBJECTIVE Calculate magnetic fields for highly symmetric current configurations using Ampere’s Law (STEM12_GPEM-IIIi-65).
  • 3. GUIDE CARD Gauss’s Law allowed us to find the net electric field due to any charge distribution by applying symmetry. Carl Friedrich Gauss Are we able to find the net magnetic field due to current if there is symmetry? Let’s get help from Ampere’s Law. AndrΓ©-Marie AmpΓ¨re
  • 4. GUIDE CARD Ampere’s Law is a useful law that relates the net magnetic field along a closed loop to the electric field current passing through the loop. First discovered by AndrΓ©-Marie AmpΓ¨re in
  • 5. GUIDE CARD The integral around a closed path of the component of the magnetic field tangent to the direction of the path is equals to Β΅ times the current I intercepted by the area within the path. 𝐡. 𝑑𝑠 = πœ‡0 𝐼𝑒𝑛𝑐
  • 6. GUIDE CARD 𝐡. 𝑑𝑠 = πœ‡0 𝐼𝑒𝑛𝑐 line integral B.ds is integrated around a closed loop called Amperian Loop Permeability of free space (constant) Enclosed current by the curve AMPERE’S LAW
  • 7. GUIDE CARD IMPORTANT NOTES - All currents have to be steady and do not change with time. -Only currents crossing the area inside the path are taken into account. -Current have to be taken with their algebraic sign by using the Right Hand Rule
  • 8. GUIDE CARD THE RIGHT HAND RULE for DETERMINING THE DIRECTION OF MAGNETIC FIELD
  • 9. ACTIVITY CARD No.1 Find the magnetic field outside a long straight wire with current I and radius r. I r Amperian Loop Wire surface Direction of Integration Magnetic field B ds r cross-section of the wire
  • 10. ACTIVITY CARD No.2 What is the direction of magnetic field due to a current passing through a solenoid? Remember to use the Right Hand Rule where the thumb takes the direction of the current.
  • 11. ACTIVITY CARD No.3 Use Ampere’s Law to determine the magnetic field strength outside a solenoid with n turns (coils) per unit length. L
  • 12. ASSESSMENT CARD No.1 Find the magnetic field inside a current- carrying wire. ds r R R I B Amperian Loop
  • 13. ASSESSMENT CARD No.2 Calculate the magnetic field B in a wire with radius 1Β΅m and the current passing through it is 1 A. Note that 𝝁 𝟎 = πŸ’π… 𝒙 πŸπŸŽβˆ’πŸ• 𝑻. π’Ž/𝑨.
  • 14. ASSESSMENT CARD No.3 The magnetic field strength of a solenoid is 0.0270T. Its radius is 0.40 m and length is 0.40 m. How many turns are there in the solenoid if the steady current passing through it is 12.0 A?
  • 15. ENRICHMENT CARD Magnetic Field of a Toroid The current enclosed by the dashed line is just the number of loops times the current in each loop. Ampere’s Law then gives the magnetic field by 𝐡 2πœ‹π‘Ÿ = πœ‡0 𝑁𝐼 𝐡 = πœ‡0 𝑁𝐼 2πœ‹π‘Ÿ
  • 16. ENRICHMENT CARDToroid is a useful device used in many applications in telecommunication, music instruments, medical field, ballasts, EMI filter among others to direct and restrict magnetic fields.
  • 17. ENRICHMENT CARD Additional Helpful Reading www.learnapphysics.com/apphysicsc/magnetism.php AP Physics C – Ampere’s Law https://www.youtube.com/watch?v=pLyrVDJ3qas&t=5s
  • 18. REFERENCE CARD AP Physics C – Amperes Law. (2013). Retrieved from https://www.youtube.com/watch?v=pLyrVDJ3qas&t=5s Elert, G. (n.d.). Ampere’s Law – Problems – The Physics Hypertextbook. Retrieved from https://physics.info/law- ampere/problems/shtml. SS: Magnetic field due to current in a straight wire. (2015). Retrieved from https://www.miniphysics.com/ss- magnetic-field-due-to-current-in-a-straight-wire.html Solenoid. (n.d.). Retrieved from http://hyperphysics.phy-astr.gsu.edu/hbase/magnetic/solenoid.html Toroidal Magnetic Field. (n.d.). Retrieved from http://hyperphysics.phyastr.gsu.edu/hbase/magnetic/toroid.html White, R. (n.d.). Learn AP Physics – Magnetism. Retrieved from http://www.learnapphysics.com/apphysicsc/magnetism.php
  • 19.
  • 20. ACTIVITY No.1 𝐡. 𝑑𝑠 = πœ‡0 𝐼 𝐡 𝑑𝑠 = πœ‡0 𝐼 𝐡 2πœ‹π‘Ÿ = πœ‡0 𝐼 𝑑𝑠 = 2πœ‹π‘Ÿ β†’ π‘π‘–π‘Ÿπ‘π‘’π‘šπ‘“π‘’π‘Ÿπ‘’π‘›π‘π‘’ π‘œπ‘“ π‘Ž π‘π‘–π‘Ÿπ‘π‘™π‘’ 𝐡 = πœ‡0 𝐼 2πœ‹π‘Ÿ
  • 21. ANSWER KEY Activity No.2: Remember that Right Hand Rule says that the thumb takes the direction of the current and the curl of the palm is the direction of the magnetic field. Thus, in this case, the magnetic field is like passing through the solenoid.
  • 22. ANSWER KEY Activity No.3: 𝑩. 𝒅𝒔 = 𝝁 𝟎 𝑰 𝑩 𝒅𝒔 = 𝝁 𝟎 𝑰 𝒅𝒔 = 𝑳 β†’ 𝒕𝒐𝒕𝒂𝒍 π’π’†π’π’ˆπ’•π’‰ 𝒐𝒇 𝒕𝒉𝒆 π’˜π’Šπ’“π’†(π’”π’π’π’†π’π’π’Šπ’…) 𝑰 β†’ 𝒏𝑰 π’‚π’Žπ’π’–π’π’• 𝒐𝒇 𝒄𝒖𝒓𝒓𝒆𝒏𝒕 𝒅𝒖𝒆 𝒕𝒐 π’π’–π’Žπ’ƒπ’†π’“ 𝒐𝒇 𝒕𝒖𝒓𝒏𝒔 𝑩 𝑳 = 𝝁 𝟎 𝒏𝑰 ∴ 𝑩 = 𝝁 𝟎 𝒏𝑰 𝑳 β†’ π’Žπ’‚π’ˆπ’π’†π’•π’Šπ’„ π’‡π’Šπ’†π’π’… π’Šπ’ 𝒂 π’”π’π’π’†π’π’π’Šπ’…
  • 23. ANSWER KEY Assessment No.1: 𝐡. 𝑑𝑠 = πœ‡0 𝐼 𝐡 𝑑𝑠 = πœ‡0 𝐼 𝐡 2πœ‹π‘Ÿ = πœ‡0 𝐼 𝑑𝑠 = 2πœ‹π‘Ÿ β†’ π‘π‘–π‘Ÿπ‘π‘’π‘šπ‘“π‘’π‘Ÿπ‘’π‘›π‘π‘’ π‘œπ‘“ π‘Ž π‘π‘–π‘Ÿπ‘π‘™π‘’ 𝐼𝑒𝑛𝑐 = πœ‹π‘Ÿ2 𝑖 πœ‹π‘…2 β†’charge enclosed is proportional to the area encircled by the loop 𝐡 (2πœ‹π‘Ÿ) = πœ‡0 πœ‹π‘Ÿ2 𝑖 πœ‹π‘…2 ∴ 𝐡 = πœ‡0 πΌπ‘Ÿ 2πœ‹π‘…2 β†’ π‘šπ‘Žπ‘”π‘›π‘’π‘‘π‘–π‘ 𝑓𝑖𝑒𝑙𝑑 𝑖𝑛 π‘Ž π‘π‘œπ‘Žπ‘₯π‘–π‘Žπ‘™ π‘π‘Žπ‘π‘™π‘’
  • 24. ANSWER KEY Assessment No.2: 𝐡 = (4πœ‹ π‘₯ 10βˆ’7 𝑇. π‘š/𝐴)(1𝐴) (2πœ‹)(1 π‘₯ 10βˆ’3 π‘š) 𝐡 = 200 πœ‡π‘‡
  • 25. ANSWER KEY Assessment No.3: 𝐡 = πœ‡0 𝑁𝐼 𝐿 𝑁 = 𝐡𝐿 πœ‡0 𝐼 𝑁 = 𝐡𝐿 πœ‡0 𝐼 = (0.0270 𝑇)(0.40 π‘š) (4πœ‹ π‘₯ 10βˆ’7 𝑇.π‘š/𝐴)(12 𝐴) = 716 π‘‘π‘’π‘Ÿπ‘›π‘ 
  • 26. ONLINE VERSION This SIM is also available online via Slideshare on this link: