Figure 26–79 shows the circuit for a simple sawtooth oscillator . At time t = 0, its switch S is closed. The neon bulb has initially infinite resistance until the voltage across it reaches 90.0 V, and then it begins to conduct with very little resistance (essentially zero). It stops conducting (its resistance becomes essentially infinite) when the voltage drops down to 65.0 V. ( a ) At what time t 1 does the neon bulb reach 90.0 V and start conducting? ( b ) At what time t 2 does the bulb reach 90.0 V for a second time and again become conducting? ( c ) Sketch the sawtooth waveform between t = 0 and t = 0.70 s. FIGURE 26–79 Problem 90.
Figure 26–79 shows the circuit for a simple sawtooth oscillator . At time t = 0, its switch S is closed. The neon bulb has initially infinite resistance until the voltage across it reaches 90.0 V, and then it begins to conduct with very little resistance (essentially zero). It stops conducting (its resistance becomes essentially infinite) when the voltage drops down to 65.0 V. ( a ) At what time t 1 does the neon bulb reach 90.0 V and start conducting? ( b ) At what time t 2 does the bulb reach 90.0 V for a second time and again become conducting? ( c ) Sketch the sawtooth waveform between t = 0 and t = 0.70 s. FIGURE 26–79 Problem 90.
Figure 26–79 shows the circuit for a simple sawtooth oscillator. At time t = 0, its switch S is closed. The neon bulb has initially infinite resistance until the voltage across it reaches 90.0 V, and then it begins to conduct with very little resistance (essentially zero). It stops conducting (its resistance becomes essentially infinite) when the voltage drops down to 65.0 V. (a) At what time t1 does the neon bulb reach 90.0 V and start conducting? (b) At what time t2 does the bulb reach 90.0 V for a second time and again become conducting? (c) Sketch the sawtooth waveform between t = 0 and t = 0.70 s.
In the circuit shown in the figure, the S switch closed at t=0 and the capacitors, which are completely empty, begin to fill. Here ε=10 V, C=5 μF and R=55 Ω.
What is the time constant of the circuit, τ, in units of microseconds?
When t= τ, what is the total charge, in units of microcoulomb, accumulated in the capacitors?
(b)
Two units of DC voltmeters, A and B are used to measure a voltage from a resistor R2 as in
Figure Q4 (b).
These instrument specifications are stated as below:
Meter A: Sensitivity S = 3 kN/V, Internal Resistance Rm = 0.5 kN, Range = 15 V
%3D
Meter B: Sensitivity S = 15 kN/V, Internal Resistance Rm = 3 kN, Range = 20 V
%3D
Ri=5kQ
30 V
RF 25k2
Figure Q4(b)
Calculate:
(i)
Voltage across R2 without any instrument connected.
(ii)
Voltage across R2 using instrument A.
(iii)
Voltage across R2 using instrument B.
(iv)
Absolute error for each measurement.
R1 is 150 ohms, and R2 is 220 ohms. (150 +220 = 370). In a series circuit, the current is the same across the circuit. The available power storage is 6 volts. The problem I am have is conceptualizing what V1 + V2 equals. I conjecture that the sum would be less than 6 V. I can't say 3 + 3 =6 V, but rather V1 + V2 < 6?
Unless R1=R2, then perhaps 3 + 3 = 6V. However, R1 is 150 ohms, and R2 is 220 ohms.
Complicating issue, if I use an ammeter and voltmeter, these devices may have some internal resistance, so equals becomes < 6 V?
How then do I conceptualize better, V1 + V2, so that maybe it is based on the value of the individual Resistor?
Chapter 26 Solutions
Physics for Scientists and Engineers with Modern Physics
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