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In the following circuit the thermistor NTC has at and .
The digital voltmeter (DVM), measuring the output , indicates . Obtain the temperature at the thermistor in °C.
Consider the following circuit in which the thermistor NTC has at and .
Determine the output voltage when the temperature is .
The Wien bridge shown in the figure is used as a null frequency detector when driven by an ac voltage.
Adjusting and , there is a null detection observed when and .
The standard capacitors (fixed-value) are , and .
Determine the detected null frequency.
Consider the following Maxwell inductance bridge circuit used to characterize the inductance modeled as the self-inductance and its equivalent series resistance .
By properly adjusting the variable resistor and the variable self-inductance , the bridge is kept in equilibrium at , i.e. .
Under these circumstances, .
As for the inductor , its equivalent series resistance is .
Estimate the ratio between the unloaded quality factors of the inductors and (without in ), i.e. .
The Schering bridge shown in the figure is used to characterize a capacitor modeled by its value and equivalent series resistance .
Assuming bridge equilibrium conditions, and . The standard fixed-value components are and .
Determine the equivalent series resistance value .
In order to characterize a capacitor at , both and were adjusted to achieve equilibrium on the Schering bridge shown below. The capacitor to be characterized is modeled by its capacitance value and equivalent series resistance .
Under bridge equilibrium conditions, and . The standard fixed-value components are and .
Determine the dissipation factor (loss tangent, ) of the capacitor to be characterized.
Consider the following Hay bridge for inductance measurements.
Suppose that and were adjusted ( and ) to achieve bridge equilibrium at , i.e., .
The standard fixed-value components are and .
Determine the value of the inductor, .
For the Hay bridge shown in the figure, assuming the bridge is in equilibrium, at the frequency of , calculate the series parasitic resistance of the inductor, , considering , , , and .
The Maxwell inductance bridge shown in the figure was used to characterize the inductance under test, modeled as the self-inductance and the respective equivalent series resistance .
The bridge achieves equilibrium by adjusting the variable resistor and the variable self-inductance . The resultant values for these components are and .
The standard resistances have values and , and for inductor , its equivalent series resistance is .
Calculate the self-inductance .
For the Maxwell-Wien bridge shown in the figure in equilibrium (null detection between terminals and ) the values of the variable components are and . The fixed-value components are and .
Calculate the self-inductance .