Basic Electrical Theory
Basic Electrical Theory
Decibels, Amplification and Attenuation
The input to an amplifier is 1 volt rms and the output 10 volt rms. This is an increase of
Correct answer: 20 dB
Voltage gain in decibels is calculated using:
\[ \mathrm{Gain(dB)} = 20 \log_{10}\!\left(\frac{V_{out}}{V_{in}}\right) \]
Here, the voltage increases from \(V_{in} = 1\ \mathrm{V_{rms}}\) to \(V_{out} = 10\ \mathrm{V_{rms}}\), giving a ratio of:
\[ \frac{V_{out}}{V_{in}} = 10 \]
Substituting:
\[ \mathrm{Gain} = 20 \log_{10}(10) = 20 \times 1 = 20\ \mathrm{dB} \]
Therefore, increasing the voltage from 1 V rms to 10 V rms is a 20 dB increase.
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The input to an amplifier is 1 volt rms and output 100 volt rms. This is an increase of
Correct answer: 40 dB
Voltage gain in decibels is calculated using:
\[ \mathrm{Gain(dB)} = 20 \log_{10}\!\left(\frac{V_{out}}{V_{in}}\right) \]
Here, the voltage increases from \(V_{in} = 1\ \mathrm{V_{rms}}\) to \(V_{out} = 100\ \mathrm{V_{rms}}\), giving a ratio of:
\[ \frac{V_{out}}{V_{in}} = 100 \]
Substituting:
\[ \mathrm{Gain} = 20 \log_{10}(100) = 20 \times 2 = 40\ \mathrm{dB} \]
Therefore, increasing the voltage from 1 V rms to 100 V rms is a 40 dB increase.
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An amplifier has a gain of 40 dB. The ratio of the rms output voltage to the rms input voltage is
Correct answer: 100
Voltage gain in decibels is given by:
\[ \text{Gain (dB)} = 20 \log_{10}\left(\frac{V_{\text{out}}}{V_{\text{in}}}\right) \]
Given:
\[ 40 = 20 \log_{10}\left(\frac{V_{\text{out}}}{V_{\text{in}}}\right) \]
Dividing both sides by 20:
\[ 2 = \log_{10}\left(\frac{V_{\text{out}}}{V_{\text{in}}}\right) \]
Taking the antilog:
\[ \frac{V_{\text{out}}}{V_{\text{in}}} = 10^2 = 100 \]
Therefore, the voltage ratio is 100.
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A transmitter power amplifier has a gain of 20 dB. The ratio of the output power to the input power is
Correct answer: D — 100
A gain of 20 dB expressed as a power ratio uses the decibel power formula. Every 10 dB represents a factor of 10 in power, so 20 dB represents 10 × 10 = 100. More formally:
\[ \text{Gain (dB)} = 10 \log_{10}\!\left(\frac{P_{\text{out}}}{P_{\text{in}}}\right) \]
Rearranging to find the power ratio:
\[ \frac{P_{\text{out}}}{P_{\text{in}}} = 10^{\,\text{Gain(dB)}/10} \]
Substituting 20 dB:
\[ \frac{P_{\text{out}}}{P_{\text{in}}} = 10^{20/10} = 10^{2} = 100 \]
Therefore, a 20 dB power gain means the output power is exactly 100 times the input power.
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An attenuator network comprises two 100 ohm resistors in series with the input applied across both resistors and the output taken from across one of them. The voltage attenuation of the network is
Correct answer: 6 dB
Two equal resistors in series form a simple voltage divider. With \(100\ \Omega + 100\ \Omega\), the input voltage is split equally across the two resistors. The output taken across one resistor is therefore half of the input voltage:
\[ \frac{V_{out}}{V_{in}} = \frac{1}{2} \]
Voltage attenuation in decibels is calculated as:
\[ \mathrm{Attenuation(dB)} = 20 \log_{10}\!\left(\frac{V_{out}}{V_{in}}\right) \]
Substituting:
\[ 20 \log_{10}(0.5) \approx -6\ \mathrm{dB} \]
(The negative sign indicates attenuation.)
Therefore, the voltage attenuation of the network is approximately 6 dB.
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An attenuator network has 10 volt rms applied to its input with 1 volt rms measured at its output. The attenuation of the network is
Correct answer: 20 dB
Voltage attenuation in decibels is calculated using:
\[ \mathrm{Attenuation(dB)} = 20 \log_{10}\!\left(\frac{V_{out}}{V_{in}}\right) \]
Here, the input voltage is \(V_{in} = 10\ \mathrm{V_{rms}}\) and the output voltage is \(V_{out} = 1\ \mathrm{V_{rms}}\), giving a ratio of:
\[ \frac{V_{out}}{V_{in}} = \frac{1}{10} = 0.1 \]
Substituting:
\[ 20 \log_{10}(0.1) = 20 \times (-1) = -20\ \mathrm{dB} \]
The negative sign indicates attenuation, so the magnitude of the attenuation is 20 dB.
Therefore, reducing the voltage from 10 V rms to 1 V rms corresponds to an attenuation of 20 dB.
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An attenuator network has 10 volt rms applied to its input with 5 volt rms measured at its output. The attenuation of the network is
Correct answer: 6 dB
Voltage attenuation in decibels is given by:
\[ \text{Attenuation (dB)} = 20 \log_{10}\left(\frac{V_{\text{in}}}{V_{\text{out}}}\right) \]
Given:
Substituting:
\[ \text{Attenuation} = 20 \log_{10}\left(\frac{10}{5}\right) = 20 \log_{10}(2) \approx 20 \times 0.301 \approx 6\ \mathrm{dB} \]
Therefore, the attenuation is 6 dB.
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Two amplifiers with gains of 10 dB and 40 dB are connected in cascade. The gain of the combination is
Correct answer: 50 dB
When amplifiers are connected in cascade, their gains in decibels add directly:
\[ G_{\text{total}} = G_1 + G_2 \]
Given:
So:
\[ G_{\text{total}} = 10 + 40 = 50\ \mathrm{dB} \]
Therefore, the total gain is 50 dB.
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An amplifier with a gain of 20 dB has a -10 dB attenuator connected in cascade. The gain of the combination is
Correct answer: B — 10 dB
When stages are connected in cascade, their gains and losses in decibels are simply added algebraically. An attenuator introduces a negative gain (a loss), so combining a +20 dB amplifier with a −10 dB attenuator gives an overall gain of:
\[ G_{\text{total}} = G_{\text{amplifier}} + G_{\text{attenuator}} \]
\[ G_{\text{total}} = 20\ \text{dB} + (-10\ \text{dB}) = 10\ \text{dB} \]
This is one of the key advantages of the decibel scale — cascaded stages can be combined by simple addition rather than multiplication of power ratios.
Therefore, the gain of the combination is 10 dB, found by algebraically adding the amplifier gain and attenuator loss in decibels.
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Each stage of a three-stage amplifier provides 5 dB gain. The total amplification is
Correct answer: 15 dB
When amplifier stages are cascaded, gains in decibels add directly.
Given:
Total gain:
\[ G_{\text{total}} = 5 + 5 + 5 = 15\ \mathrm{dB} \]
Therefore, the total amplification is 15 dB.
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