2014年6月2日 星期一

Day 23 Inductors

Inductors:


In this lab we were ask to set up a a circuit, which include inductor and resistance and function generator.
Umm~ Calculation Error ~ correct one will be posted later.
Below is the gotten data:

2014年5月28日 星期三

Day 22 Solenoids

Solenoids:


This experiment we use plastic tube and wrapped wire to attach the power supply with a coil.
Begin with 1 loop and increase 1 loop at once till 5 loops.
We set magnetic field sensor inside the tube to make sure sensor is below( we didn't do above) the center of coil. 
Result below:

As the result, we can see the ratio of the magnetic field is decrease as loop increase, and it drop till 3.5*10^-5 T/A.
By using this value we can calculated the length of wire by formula below (Solenoid)


Magnet in Motion:

We connect this large coil to ammeter to induce current. We discover the relationship below


========================================================================
Extra Credit

========================================================================

















2014年5月19日 星期一

Day 21 Earth's Magnetic Field

Magnetic Field of Earth:

We set up the tool above to determine the magnetic field of the Earth.

Using Biot-Savart Law we calculated the magnetic field for the coil using current, the number of coil turns, radius and the constant.
Then we used the relationship between Earth field, and coil field to determine the field.
We determined by using the compass changing degree and known current to solved for the magnetic field of Earth by dividing the magnetic field of the coil by tangent theta. As the graph below we knew that the slope of the data set would be the magnetic field of the earth.
 

2014年5月13日 星期二

Day 20 Motor



Magnetic Motor:


With Power supply the magnetic motor spin clock-wisely.


Switch the magnetic cause it spin counter wisely.

Self-Made Magnetic Motor:


Over here, we create our own magnetic motor with copper wires, paper clip, Disney cup,magnetic, and power supply.
First, we wrapped wire to get a symmetric circular.
Second, we used sand paper to sanded 180 degree for one end of wire, and 360 degree for another end of wire.
Third, We attached paper clip to the bottom of cup and place magnetic in the center.
Forth, attach power supply to the paper clip and set the symmetric circular wire on the paper clip.
Last, turn the power supply on, and let it spin.









2014年5月12日 星期一

Day 19 Magnetic Field

Magnetic Field:

By using compass, we can see the magnetic vector in each position, and the result is magnetic vector goes out at south back at north.
Using this we can easily seem the magnetic filed by steal powder.
These three graph show the magnetic field is similar to electric field but represent differently. It represent positive and negative with north and south.  


Vector relationship between F,v,and B




As we know, the magnetic force is equal to I (current) * l (distance) "CROSS" B (magnetic field).
In order to solve B we can replace force by ma + mr^2; however, even we solve the answer, the unit become confusing.

Magnetic Field involve rotation:

Here comes the rectangle wire relationship that magnetic field crossed in two different ways.

Here comes the calculation of magnetic filed under X-Y-Z vectors.


2014年5月7日 星期三

Day 18 Transistor

Transistor and amplifier

We were asked to build a electric circuit~!!
With above setup and amplifier 3kHZ, frequency 0.3 V with 2N3904 transistor, we got the graph below.

Here comes two waves by function generator.
It shows original V as 0.3 V and another one above with 20V~30V.
It means the set up one has 100 times bigger than original.

Semiconductor Lab:

Using the graph above to set up the circuit.
This is the setup we finally be able to here the music