Friday, 29 March 2013

GATE PROBLEM


Friday, 29 March 2013 by Unknown · 0

Monday, 25 March 2013

RC FOSTER FORM - 2



Monday, 25 March 2013 by Unknown · 0

Sunday, 24 March 2013

RC IMPEDANCE FOSTER FORM 1



Sunday, 24 March 2013 by Unknown · 2

Saturday, 23 March 2013

CAUER FORM 2 LC IMMITTANCE






Saturday, 23 March 2013 by Unknown · 0

CAUER FORM 1 LC IMMITTANCE




by Unknown · 0

FOSTER FORM 2 FOR LC IMMITTANCE




by Unknown · 0

FOSTER FORM I FOR LC IMMITTANCE




by Unknown · 0

Friday, 22 March 2013

RL IMPEDANCE OR RC ADMITTANCE


PROPERTIES OF RL IMPEDANCE OR RC ADMITTANCE
1) Poles and zeros are alternating
2) Poles and zeros are simple and lie on the negative real axis of the s-plane.
3)The critical frequency nearest to origin is a zero
4) The critical frequency farthest from origin is a pole
5)The residues of Y(s) at its poles are all negative and real
6) The slope of YRC(σ) is positive and the slope of YRC(-σ) is negative
7) YRC(∞)≥YRC(0) 

Methods for realising a RC IMPEDANCE OR RL ADMITTANCE function

1) Foster form 1

2) Foster form 2

3) Cauer form 1

4) Cauer form 2

FOSTER FORM 1
It is used to realize impedance function.


Read more »

Friday, 22 March 2013 by Unknown · 0

Thursday, 21 March 2013

RC impedance or RL admittance



PROPERTIES OF RC IMPEDANCE OR RL ADMITTANCE

1)Poles and zeros are alternating

2) Poles and zeros are simple and lie on the negative real axis of the s-plane.

3)The critical frequency nearest to origin is a pole which indicates a capacitor for RC impedance

4) The critical frequency farthest from  origin is a zero which indicates a capacitor for RC impedance

5)The residues of Z(s) at its poles are all positive and real

6) The slope of ZRC(σ) is negative and the slope of ZRC(-σ) is positive
7) ZRC(0) ≥ZRC(∞)

Methods for realising a RC IMPEDANCE OR RL ADMITTANCE function

1) Foster form 1

2) Foster form 2

3) Cauer form 1

4) Cauer form 2

FOSTER FORM 1
It is used to realize impedance function. 

Read more »

Thursday, 21 March 2013 by Unknown · 0

Tuesday, 19 March 2013

DUAL SLOPE INTEGRATING TYPE DVM



Switch connected to +VM

Once VM is connected, the capacitor starts charging linearly then the output at the integrator decreases linearly. This linearly decreasing ramp is fed to inverting terminal of the zero crossing detector. Since the input at non inverting terminal is greater than inverting terminal, it produces a positive going pulse. This positive going pulse makes the gating circuit to start. Now pulses produced by the clock generator passess through gating circuit and counter count the number of pulses.
                                 t
                 VC = 1/C  ∫ I dt
                            -∞
                                 t1
                       = 1/C ∫ VM / R dt
                              0

                       =   VM / RC ( t1 – 0 )

                       =   VMt1/RC

                       =   VMT1/RC (t1 =T1)

                  V0 = -VC

                  V0 = - ( VMT1/RC )

Graphs of VC and V0

Read more »

Tuesday, 19 March 2013 by Unknown · 0

Sunday, 17 March 2013

CONTENTS OF EDC

Sunday, 17 March 2013 by Unknown · 0

CONTENT OF EMI

TO READ THE SPECIFIC TOPIC CLICK ON THE LINK GIVEN BY THE SIDE OF EACH TOPIC
 
INTRODUCTION TO DVMs 
DIGITAL READOUTS OF DVMs 
TYPES OF DVMs
    RAMP TYPE 
    DUAL SLOPE INTEGRATING TYPE

by Unknown · 0

RAMP TYPE DVM


IT IS ALSO CALLED SINGLE SLOPE TYPE DVM OR PULSE WIDTH TYPE DVM
OPERATION

This DVM measures unknown voltage VM by measuring the time taken by a linearly falling ramp voltage to fall from unknown voltage level to zero volts

Ramp generator produces a decreasing OR increasing ramp

Input comparator generates starting pulse to open gate circuit

Output generator produces stop pulse to close gate circuit

Clock generator produces pulses

Decade counter calculates number of pulses that pass through it

AT INPUT COMPARATOR
An unknown voltage VM is given to the input of non inverting terminal. When the input at inverting terminal of op-amp is less than VM out at the input comparator is positive otherwise it is negative. When VR decreases below VM it produces a positive going pulse, this pulse makes the gating circuit to start and the pulse produced by the clock generator passes through the gating circuit. These pulses are counted by decade counter

AT GROUND COMPARATOR 
Ground comparator or zero level detector .so when the VR crosses zero and moves to negative values, the input at inverting terminal is greater than non inverting terminal. So output of this comparator produces a negative going pulse which makes the gating circuit to stop. Therefore the reading displayed on the display is the unknown voltage.
VOLTAGE TO TIME CONVERSION 

VR ------------TR
VM ----------TM
VM = ( VR / TR )*TM
Time period measurement
Let  TCLK be time period of clock generator. Let ‘n ‘ be the number of clock pulses between T1 and T2
T2 – T1 = TM = n* TCLK
Substitute the value of TM in VM we get
VM = ( VR / TR )* n *TCLK

FEATURES OF RAMP TYPE DVM
1)CONVERSION TIME
                 TCONV = TM = nTCLK 
Where n is proportional to | VM | because the number of pulses depends upon VM
2) NOISE REJECTION
If either AC signal or noise is superimposed on unknown DC voltage then error is introduced in voltage measurement. So noise affect is more. Therefore noise rejection is poor. Since stability of DVM depends on noise condition. Its stability is poor.
3) ACCURACY
Value Internal components of ramp generator changes due to aging then linearity of ramp changes then VM also changes as shown in the figure and accuracy of measurement is affected.




by Unknown · 0

Saturday, 16 March 2013

DEFINITIONS IN A WAVE FORM


                         The sinusoidal waveform of figure 1 with its additional notation will now be used as a model in defining a few basic terms. These terms, however, can be applied to any alternating waveform. It is important to remember as you proceed through the various definitions that the vertical scaling is in volts or amperes and the horizontal scaling is always in units of time.

Waveform
The path traced by a quantity, such as the voltage in figure 1, plotted as a function of some variable such as time (as above), position, degrees, radians, temperature, and so on.

Instantaneous value
The magnitude of a waveform at any instant of time; denoted by lowercase letters (e1, e2).

Read more »

Saturday, 16 March 2013 by Unknown · 0

READ OUTS OF DVMs



In 3 / 4 digit numerator indicates maximum value and denominator indicates number of digits


Number of digits
Maximum value
9/10
0,1,2,3………9
9
1/2
0,1
1
3/4
0,1,2,3
3
Note
A full digit has decimal point but ½ , ¾ … doesn’t have decimal point
Example
( 0 – 1 )V 3 digit DVM
SOLUTION

Read more »

by Unknown · 0

Sample Links

All Rights Reserved ECE | Blogger Template by Bloggermint