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[object Object],[object Object],[object Object],[object Object]
Benefits of Understanding Electricity ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
The Atom ,[object Object],[object Object],[object Object],[object Object],[object Object]
Free Electrons & Current ,[object Object],[object Object],[object Object]
Conductors & Insulators ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Static Electricity ,[object Object],[object Object],[object Object],[object Object]
Static Electricity Demonstration ,[object Object],[object Object],[object Object],[object Object],[object Object]
Current, Voltage, Resistance ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Coulombs Law of Charges ,[object Object],[object Object],[object Object]
Water Example of Electric Circuit ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Ohms Law ,[object Object],[object Object],[object Object],[object Object],[object Object],E E I R
Circuit Diagrams Battery (short side is negative terminal) Resistor Light bulb (or other load) Open switch Closed switch Wire conductor Ground
Series Circuit Analysis 4v 2  E = IR 4v = I * 2   I = 2a A 4v battery is placed in a series circuit with a 2   resistor.   What is the total current that will flow through the circuit? I = ?
Series Circuit Analysis ? 3  E = IR E = 2a * 3  E = 6v What voltage is required to produce 2a though a circuit with a 3   resistor.  I = 2a
Series Circuit Analysis 12v 3  E = IR 12 = 4a * R R = 3  What resistance is required to limit the current to 4a if a 12 v battery is in the circuit?  I = 4a
Series Circuit Analysis 12v 4  E = IR 12 = I * (2   + 4  ) I = 2a Resistance in series sum together when calculating total resistance   What is the current in the circuit below? I = ? 2 
Series Circuit Analysis 12v E = IR 12 = 4 * (2   + R) R = 1  Resistance in series sum together when calculating total resistance   What is the resistance of the light bulb? I = 4 2  R = ?
Kirchhoff’s Law of Voltages ,[object Object],[object Object],[object Object],12v 4v 12v 0v -8v -4v 12v 4  I = 2 2 
Kirchhoff’s Law of Voltages ,[object Object],[object Object],24v 4  1  c d 3  a b I = 3 -9v -12v -3v a vs. d= 24v b vs. d= 15v c vs. d= 3v
Series vs. Parallel Circuits ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
By Analogy: Series Vs Parallel E I E R 1 R 2 R 3 I 1 I 2 I 3 R 1 R 2
Parallel Circuits 5  10  30  1.  First calculate total resistance 1  =  1  +  1  +  1  R tot   5   10   30 1  =  1 R tot   .333 R tot  = 3   30v What is the total current below? 2.  Then use E = IR 30v = I * 3   I = 10a
Parallel Circuits 5  10  30  30v What is the current through a? What is the current through e? What is the current  each branch b-d? a e I tot  = 10a b c d 10a 10a Same voltage is across each path b:  E= IR 30= I*5  I= 6a c:  30= I*10 I= 3a d:  30= I*30 I= 1a
Shortcuts to Total R in Parallel 30  30  30  30v If all N branches have the same resistance, total resistance is equal to the resistance of one branch divided by the number of branches Total resistance= Total current= Current in b= a e b c d 10  3a 1 
Shortcuts to Total R in Parallel 12  4  30v If there are only two branches, the total resistance is equal to the product of the resistances divided by the sum of the resistances Total resistance=  12 * 4   = 3   12 + 4
Compound Circuits 3  6  2  20v ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],e d a b c
Compound Circuits 3  6  2  20v ,[object Object],[object Object],[object Object],[object Object],e d a b c
Compound Circuits 3  6  2  20v Total current: E = I*R 20v = I * 4   I tot  = 5a e d a b c
Compound Circuits 3  6  2  20v ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],e d a b c I tot = 5a
Compound Circuits 3  6  2  20v ,[object Object],[object Object],[object Object],[object Object],e d a b c I tot = 5a
More Practice Simplifying Parallel Circuits 2  12  10  5  9  8  1. 2  24  8  12  2.
More Practice Simplifying Parallel Circuits 2  24  8  12  2. 2  6  12  3. 20  4.
Some Intuitive Questions (and Answers) V 20  10  I 30  In the following circuit with source voltage V and Total current I, which resistor will have the greatest voltage across it? The resistor with the largest resistance (30   ) Which resistor has the greatest current flow through it? Same for all because series circuit If we re-ordered the resistors, what if any of this would change? Nothing would change
Some Intuitive Questions (and Answers) V 20  10  I 30  If we added a resistor in series with these, what would happen to the total resistance, total current, voltage across each resistor, and current through each resistor? Total resistance would increase Total current would decrease Voltage across each resistor would decrease (All voltage drops must still sum to total in series circuit; Kirchhoff’s law of voltages) Current through each resistor would be lower (b/c total current decreased, but same through each one)
Some Intuitive Questions (and Answers) In the following circuit with source voltage V and Total current I, which resistor will have the greatest voltage across it? All the same in parallel branches Which resistor has the greatest current flow through it? The “path of least resistance” (10  ) What else can you tell me about the current through each branch They will sum to the total I (currents sum in parallel circuits; Kirchhoff’s law of current) 10  20  30  V I
Some Intuitive Questions (and Answers) 10  20  30  V I If we added a resistor in parallel with these, what would happen to the total resistance, total current, voltage across each resistor, and current through each resistor? Total resistance would decrease Total current would increase Voltage across each resistor would still be V Current through each resistor would be higher and would sum to new total I
A Practical Application: Voltage Dividers ,[object Object],[object Object],[object Object],[object Object]
Voltage Dividers E NS Amp V Hi input impedance (R big ) ,[object Object],[object Object],[object Object]
Voltage Dividers E NS Amps V Hi input impedance (R big ) ,[object Object],[object Object],[object Object],[object Object],R 1
Voltage Dividers E NS Amps V Hi input impedance (R big ) ,[object Object],[object Object],[object Object],[object Object],R 1 R 2
Voltage Dividers E NS Amps 5K V Hi input impedance (R big ) ,[object Object],[object Object],[object Object],[object Object],[object Object],a c b 15K
Voltage Dividers E NS Amps R2 V Hi input impedance (R big ) ,[object Object],[object Object],[object Object],[object Object],a c b R1
A Practical Example: Measuring SC R2 V I R1 SR NS Amps R1 + R2 << SR We want to measure conductance (1/R) through a subject.  Explain how the circuit below accomplishes this. Voltage across R1 and subject will be equal and remain constant as SR changes (very small voltage change over R2 b/c R2 << SR) Current in subject branch is a function of SR (b/c SR >> R2) Voltage change over R2 is proportional to current in this branch E=IR) and therefore inversely proportional to SR (which is conductance)
DC Current vs. AC Current  ,[object Object],[object Object],[object Object],[object Object],[object Object],Much of this info was borrowed from: http://www.sweethaven.com/acee/forms/toc01.htm
The Sinusoidal AC Waveform  ,[object Object],[object Object],[object Object]
Instantaneous Voltage and Current ,[object Object],[object Object],[object Object],[object Object],[object Object]
Peak and Peak-to-Peak Voltage Peak voltage  is the voltage measured from the baseline of an ac waveform to its maximum, or peak, level.  Peak-to-peak voltage  is the voltage measured from the maximum positive level to the maximum negative level.
Root-Mean-Square (RMS) Voltage AC levels are assumed to be expressed as RMS values unless clearly specified otherwise. RMS voltage is the amount of dc voltage that is required for producing the same amount of power as the ac waveform.  The RMS voltage of a sinusoidal waveform is equal to 0.707 times its peak value.
Period of a Waveform ,[object Object],[object Object],[object Object],[object Object]
Frequency of a Waveform ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Phase Angle ,[object Object],[object Object],[object Object],[object Object],[object Object]
Capacitors ,[object Object],[object Object]
Charged Capacitor ,[object Object],[object Object],[object Object]
Electrostatic Induction  ,[object Object],[object Object],[object Object]
Capacitance ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Charging and Discharging ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Capacitor  Charge  and Discharge (DC) ,[object Object],[object Object],[object Object],[object Object]
Capacitor  Charge  and Discharge (DC) ,[object Object],[object Object],[object Object],[object Object]
RC Time Constant  ,[object Object],[object Object],[object Object],[object Object]
RC Charge Curve  ,[object Object],[object Object],[object Object]
RC Discharge Curve ,[object Object],[object Object],[object Object]
Capacitor Charge and Discharge (AC) Applied voltage is increasing during the positive half-cycle and current flows through the circuit clockwise to charge the plates of the capacitor. Applied voltage is decreasing during the positive half-cycle and current flows through the circuit counter-clockwise to discharge the plates of the capacitor Applied voltage is increasing during the negative half-cycle and current flows through the circuit counter-clockwise to charge the plates of the capacitor with the opposite polarity. Applied voltage is decreasing during the negative half-cycle, current flows through the circuit clockwise to discharge the plates of the capacitor
Capacitive Reactance Reactance  is the opposition to current flow presented by capacitors (and inductors) Capacitive reactance(X C )= 1 / (2    f C) Holding capacitance constant, what happens to X C  as f increases? There is less and less reactance to the current flow as the frequency of the voltage source increases In contrast, what happens to resistance across a resistor as frequency increases? It does not change
Capacitive Reactance ,[object Object],[object Object],[object Object]
Impedance In a resistive and reactive circuit, impedance is the total opposition to current in the circuit. Impedance = sqrt (R 2  + X C 2 ) Current can still be determined from voltage (using Ohms law) but need to substitute impedance for resistance when calculating total current in a circuit Total voltage drop across resistor and capacitor will not equal source voltage. Instead Vs = sqrt (V C 2  and V R 2 )
A Practical Application: Low & Hi Pass Filters Which is the low pass and which is the hi pass filter? R C
A Practical Application: Low & Hi Pass Filters How would you calculate the current in the diagrams below? Know that the total resistance = sqrt (R 2  + X C 2 ) Therefore, total current = V in  / R tot R C
A Practical Application: Low & Hi Pass Filters Is the current the same throughout the circuits? Yes, they are series circuits Which will have the higher voltage drop, the R or the C? Depends on which has the higher resistance/reactance.  The voltage will drop differentially over the R and C with the bigger drop over the bigger resistance/reactance R C
A Practical Application: Low & Hi Pass Filters Holding capacitance constant, what happens to X C  as f increases? There is less and less reactance to the current flow as the frequency of the voltage source increases X C  = 1 / (2    f C) R C
A Practical Application: Low & Hi Pass Filters What happens to resistance across a resistor as frequency increases? It does not change R C
A Practical Application: Low & Hi Pass Filters Describe the relative voltage drops across the C for low and high frequency voltage source. As the frequency increases, the relative resistance of the C vs. R will grow smaller (b/c X C  drops and R remains constant) Therefore, the relative voltage drop across the C will be greater for low than high frequency voltages R C
A Practical Application: Low & Hi Pass Filters Describe the relative voltage drops across the R for low and high frequency voltage source. As the frequency increases, the relative resistance of the R vs. C will grow larger (b/c R remains constant while X C  drops) Therefore, the relative voltage drop across the R will be smaller for low than high frequency voltages R C
A Practical Application: Low & Hi Pass Filters R C
Time constant of Low pass Filter ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Time constant of Low pass Filter ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Demo of Characteristics of a Low Pass Filter ,[object Object],[object Object],[object Object],[object Object],[object Object]
Unit Modifiers for Reference ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],Examples : 5ma = .005a 10k   = 10000  
Filters ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Hardware vs. Digital Filters ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Sampling Rate ,[object Object],[object Object],[object Object],[object Object],[object Object]
Other Steps ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]

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Electricity lecuture

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  • 12. Circuit Diagrams Battery (short side is negative terminal) Resistor Light bulb (or other load) Open switch Closed switch Wire conductor Ground
  • 13. Series Circuit Analysis 4v 2  E = IR 4v = I * 2  I = 2a A 4v battery is placed in a series circuit with a 2  resistor. What is the total current that will flow through the circuit? I = ?
  • 14. Series Circuit Analysis ? 3  E = IR E = 2a * 3  E = 6v What voltage is required to produce 2a though a circuit with a 3  resistor. I = 2a
  • 15. Series Circuit Analysis 12v 3  E = IR 12 = 4a * R R = 3  What resistance is required to limit the current to 4a if a 12 v battery is in the circuit? I = 4a
  • 16. Series Circuit Analysis 12v 4  E = IR 12 = I * (2  + 4  ) I = 2a Resistance in series sum together when calculating total resistance What is the current in the circuit below? I = ? 2 
  • 17. Series Circuit Analysis 12v E = IR 12 = 4 * (2  + R) R = 1  Resistance in series sum together when calculating total resistance What is the resistance of the light bulb? I = 4 2  R = ?
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  • 21. By Analogy: Series Vs Parallel E I E R 1 R 2 R 3 I 1 I 2 I 3 R 1 R 2
  • 22. Parallel Circuits 5  10  30  1. First calculate total resistance 1 = 1 + 1 + 1 R tot 5 10 30 1 = 1 R tot .333 R tot = 3  30v What is the total current below? 2. Then use E = IR 30v = I * 3  I = 10a
  • 23. Parallel Circuits 5  10  30  30v What is the current through a? What is the current through e? What is the current each branch b-d? a e I tot = 10a b c d 10a 10a Same voltage is across each path b: E= IR 30= I*5 I= 6a c: 30= I*10 I= 3a d: 30= I*30 I= 1a
  • 24. Shortcuts to Total R in Parallel 30  30  30  30v If all N branches have the same resistance, total resistance is equal to the resistance of one branch divided by the number of branches Total resistance= Total current= Current in b= a e b c d 10  3a 1 
  • 25. Shortcuts to Total R in Parallel 12  4  30v If there are only two branches, the total resistance is equal to the product of the resistances divided by the sum of the resistances Total resistance= 12 * 4 = 3  12 + 4
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  • 28. Compound Circuits 3  6  2  20v Total current: E = I*R 20v = I * 4  I tot = 5a e d a b c
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  • 31. More Practice Simplifying Parallel Circuits 2  12  10  5  9  8  1. 2  24  8  12  2.
  • 32. More Practice Simplifying Parallel Circuits 2  24  8  12  2. 2  6  12  3. 20  4.
  • 33. Some Intuitive Questions (and Answers) V 20  10  I 30  In the following circuit with source voltage V and Total current I, which resistor will have the greatest voltage across it? The resistor with the largest resistance (30  ) Which resistor has the greatest current flow through it? Same for all because series circuit If we re-ordered the resistors, what if any of this would change? Nothing would change
  • 34. Some Intuitive Questions (and Answers) V 20  10  I 30  If we added a resistor in series with these, what would happen to the total resistance, total current, voltage across each resistor, and current through each resistor? Total resistance would increase Total current would decrease Voltage across each resistor would decrease (All voltage drops must still sum to total in series circuit; Kirchhoff’s law of voltages) Current through each resistor would be lower (b/c total current decreased, but same through each one)
  • 35. Some Intuitive Questions (and Answers) In the following circuit with source voltage V and Total current I, which resistor will have the greatest voltage across it? All the same in parallel branches Which resistor has the greatest current flow through it? The “path of least resistance” (10  ) What else can you tell me about the current through each branch They will sum to the total I (currents sum in parallel circuits; Kirchhoff’s law of current) 10  20  30  V I
  • 36. Some Intuitive Questions (and Answers) 10  20  30  V I If we added a resistor in parallel with these, what would happen to the total resistance, total current, voltage across each resistor, and current through each resistor? Total resistance would decrease Total current would increase Voltage across each resistor would still be V Current through each resistor would be higher and would sum to new total I
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  • 43. A Practical Example: Measuring SC R2 V I R1 SR NS Amps R1 + R2 << SR We want to measure conductance (1/R) through a subject. Explain how the circuit below accomplishes this. Voltage across R1 and subject will be equal and remain constant as SR changes (very small voltage change over R2 b/c R2 << SR) Current in subject branch is a function of SR (b/c SR >> R2) Voltage change over R2 is proportional to current in this branch E=IR) and therefore inversely proportional to SR (which is conductance)
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  • 47. Peak and Peak-to-Peak Voltage Peak voltage is the voltage measured from the baseline of an ac waveform to its maximum, or peak, level. Peak-to-peak voltage is the voltage measured from the maximum positive level to the maximum negative level.
  • 48. Root-Mean-Square (RMS) Voltage AC levels are assumed to be expressed as RMS values unless clearly specified otherwise. RMS voltage is the amount of dc voltage that is required for producing the same amount of power as the ac waveform. The RMS voltage of a sinusoidal waveform is equal to 0.707 times its peak value.
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  • 62. Capacitor Charge and Discharge (AC) Applied voltage is increasing during the positive half-cycle and current flows through the circuit clockwise to charge the plates of the capacitor. Applied voltage is decreasing during the positive half-cycle and current flows through the circuit counter-clockwise to discharge the plates of the capacitor Applied voltage is increasing during the negative half-cycle and current flows through the circuit counter-clockwise to charge the plates of the capacitor with the opposite polarity. Applied voltage is decreasing during the negative half-cycle, current flows through the circuit clockwise to discharge the plates of the capacitor
  • 63. Capacitive Reactance Reactance is the opposition to current flow presented by capacitors (and inductors) Capacitive reactance(X C )= 1 / (2  f C) Holding capacitance constant, what happens to X C as f increases? There is less and less reactance to the current flow as the frequency of the voltage source increases In contrast, what happens to resistance across a resistor as frequency increases? It does not change
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  • 65. Impedance In a resistive and reactive circuit, impedance is the total opposition to current in the circuit. Impedance = sqrt (R 2 + X C 2 ) Current can still be determined from voltage (using Ohms law) but need to substitute impedance for resistance when calculating total current in a circuit Total voltage drop across resistor and capacitor will not equal source voltage. Instead Vs = sqrt (V C 2 and V R 2 )
  • 66. A Practical Application: Low & Hi Pass Filters Which is the low pass and which is the hi pass filter? R C
  • 67. A Practical Application: Low & Hi Pass Filters How would you calculate the current in the diagrams below? Know that the total resistance = sqrt (R 2 + X C 2 ) Therefore, total current = V in / R tot R C
  • 68. A Practical Application: Low & Hi Pass Filters Is the current the same throughout the circuits? Yes, they are series circuits Which will have the higher voltage drop, the R or the C? Depends on which has the higher resistance/reactance. The voltage will drop differentially over the R and C with the bigger drop over the bigger resistance/reactance R C
  • 69. A Practical Application: Low & Hi Pass Filters Holding capacitance constant, what happens to X C as f increases? There is less and less reactance to the current flow as the frequency of the voltage source increases X C = 1 / (2  f C) R C
  • 70. A Practical Application: Low & Hi Pass Filters What happens to resistance across a resistor as frequency increases? It does not change R C
  • 71. A Practical Application: Low & Hi Pass Filters Describe the relative voltage drops across the C for low and high frequency voltage source. As the frequency increases, the relative resistance of the C vs. R will grow smaller (b/c X C drops and R remains constant) Therefore, the relative voltage drop across the C will be greater for low than high frequency voltages R C
  • 72. A Practical Application: Low & Hi Pass Filters Describe the relative voltage drops across the R for low and high frequency voltage source. As the frequency increases, the relative resistance of the R vs. C will grow larger (b/c R remains constant while X C drops) Therefore, the relative voltage drop across the R will be smaller for low than high frequency voltages R C
  • 73. A Practical Application: Low & Hi Pass Filters R C
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