These are the regions that the transitors works and what they are cutoff is where there is little electron flow through the connections. active is where electron flow can vary quite a bit but when in saturation the switch is fully turned on. Also varying the voltage of the transistor you can change the amount of beta.
Thursday, August 19, 2010
Experiment #7
These are the regions that the transitors works and what they are cutoff is where there is little electron flow through the connections. active is where electron flow can vary quite a bit but when in saturation the switch is fully turned on. Also varying the voltage of the transistor you can change the amount of beta.
Experiment #6
Wednesday, August 18, 2010
Experiment #4
Sunday, August 15, 2010
Experiment #3
this shows that higher the voltage the higher the voltage drop across the diode but by only a small amount. I then made a smaller circuit with 1 resistor = 1K and switched between a L.E.D and a 1N4007 rectifier diode shown in this circuit below and datasheet.
Calculated and Measured Amperage
Calculated = 0.0043mA (5V - .7V/1000 = 0.0043mA)
Measured = 0.004mA
this is because the amps calculation in the circuit is a estimate of the amperage and will be close to the real value.
Calculated and Measured Voltage drop across diode
Calculated = .7V (general specifications)
Measured = .654V
this is because .7 is its max voltage drop it has.
Then added a L.E.D instead of the rectifier diode
Calculated Current = 0.0032mA (5v - 1.8v/1000 = 0.0032ma)
Measured Current = 0.0038mA
Saturday, August 14, 2010
Experiment #5 Capacitors
- Non -Electrolytic Capacitor
- Variable Capacitor
- Electrolytic Capacitor
- Tantalum Capacitor
Circuit Capacitor Charging Circuit
Calculated = 330uf with 1k resistor (0.033 x 1000 = 33 mS)
Saturday, August 7, 2010
Diodes - Rectifier, Zener and L.E.D
Wednesday, July 28, 2010
Resistors in Series and Parallel circuits
When a resistor is put in parallel into a circuit it works differently to when its put in series. When it is in series all the resistances can be added together to give a total resistance but with parallel circuits it is the number that can be divided equally into each resistance divided by the largest resistance in the ciruit which will give you reisistance. The two formulas are set out like this
Series
Parallel