1. What happens to the distribution of magnetic flux lines when the iron ring was placed in between the U-magnets?
The distribution of magnetic flux lines when the iron ring is placed in between the magnets, the iron ring is included in the distribution of flux lines. Instead of connecting to the other pole, the ring affects its distribution and some of it is attracted to the iron ring.
2. How does changing the current affect the magnetic force on a wire suspended in a magnetic field?
As the current rises, the magnetic force is pushing the magnet away from the current, or pulls the magnet either it is north pole of south pole. The force is increasing as the current increases.
3. What would happen if the magnets in the assembly were not properly arrange, meaning the North Pole of one of the magnets is right next to the S pole of the other magnet?
There will be a change in the distribution of forces, since, the North Pole and South Pole attract each other, and therefore, it will change the magnetic force and have error in the experiment.
4. What is the effect of changing the orientation of the loop of wires in the last part of the experiment? What orientation gives the maximum magnetic force? The minimum force?
The effect of changing the orientation of the loops makes the magnet being repelled or attracted by the current. The maximum force is the highest angle whose magnetic force is 9.8×10-3 N in both repulsion and attraction. The minimum force is the angle 0 who do not have angle force produce because the orientation of the current and the magnetic force is parallel to each other.
The Business plan on Channels of Distribution 3
Once you have selected and developed a unique product or business idea, correctly positioned and targeted it to buyers, and developed your packaging and pricing, the selection of distribution channels and sales representation is key to successful marketing. It’s fairly easy to change many of your marketing tactics and strategies on a periodic basis; pricing, packaging, and product mix are ...
Mapúa Institute of Technology
Department of Physics
Name: Olivete, Jasper Ryan L.
Program/Year: ChE/2
Course Code/Section: Phy140L/A4
Student No.: 2005103207
Group No.: 4 Seat No.: 404 2
Date of Performance: April 26, 2007 2
Date of Submission: May 3, 20072
Engineer Bobby (Dionisio) Manlapig
Instructor
Sample Computation:
Part 2: Magnetic Force on current-carrying conductor
a.) Magnetic Force and Magnetic Field
Current(I)
Current Loop
Number of magnets
Magnetic force in gram
5 Amps
SF 37
2
0.3 gram
Magnetic Force in Newton:
b.) Magnetic Force and Current
Current(I)
Current Loop
Magnetic force in gram
0 Amps
SF 42
0 gram
Magnetic Force in Newton:
c.) Magnetic Force and Length of current loop
Current(I)
Current Loop
Length, L
Magnetic force in gram
2 Amps
SF 40
1.2 cm
0.1 gram
Magnetic Force in Newton:
d.) Magnetic Force and orientation of coil
Current(I)
Angle, θ
Magnetic force in gram
2 Amps
0o
0 gram
Magnetic Force in Newton:
Sample Computation:
Part 2: Magnetic Force on current-carrying conductor
a.) Magnetic Force and Magnetic Field
Current(I)
Current Loop
Number of magnets
Magnetic force in gram
5 Amps
SF 37
2
0.3 gram
Magnetic Force in Newton:
b.) Magnetic Force and Current
Current(I)
Current Loop
Magnetic force in gram
0 Amps
SF 42
0 gram
Magnetic Force in Newton:
c.) Magnetic Force and Length of current loop
Current(I)
Current Loop
Length, L
Magnetic force in gram
2 Amps
SF 40
1.2 cm
0.1 gram
Magnetic Force in Newton:
d.) Magnetic Force and orientation of coil
The Term Paper on Magnetic Field Current Magnet Value
Magnatism & the Things We THINK We Know About It! By Austin D. Ritchie Magnatism is a wondrous natural phenomenon. Since days before scientific discoveries were even written down the world has been playing with the theories of magnetism. In these three labs we debt with some of the same ideas which have pondered over for long before any of us were around. In these conclusions we will take a ...
Current(I)
Angle, θ
Magnetic force in gram
2 Amps
0o
0 gram
Magnetic Force in Newton:
