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Question

A digital counter increments its count every $0.1\ \mu\text{s}$. The counter is used in an instrument to measure frequency. The counter is operated for one period of the input signal to the instrument to measure its frequency. The input signal is approximately at $100\text{ kHz}$. The maximum error in the measured frequency is _____ kHz. 

(rounded off to the nearest integer)

Frequency Counter Error Analysis

The problem asks for the maximum error in a frequency measurement performed by a digital counter. We are given the counter's time resolution and the approximate frequency of the input signal.

Understanding Measurement Parameters

  • Input Signal Frequency: $f_{in} \approx 100\ \text{kHz} = 100 \times 10^3\ \text{Hz}$.
  • Counter Resolution: The counter increments every $0.1\ \mu\text{s}$. This value represents the smallest time interval the counter can resolve, thus defining the accuracy of any time measurement it performs. Let this be $\Delta t = 0.1\ \mu\text{s} = 0.1 \times 10^{-6}\ \text{s}$.
  • Measurement Method: The counter measures the period ($T$) of the input signal. The frequency is then calculated as $f = 1/T$.

Calculating Period and Error

First, calculate the period ($T$) of the input signal:

$ T = \frac{1}{f_{in}} = \frac{1}{100 \times 10^3\ \text{Hz}} = 10 \times 10^{-6}\ \text{s} = 10\ \mu\text{s} $

The counter measures this period $T$. The maximum error in the period measurement ($\Delta T$) is equal to the counter's resolution:

$ \Delta T = \pm \Delta t = \pm 0.1\ \mu\text{s} = \pm 0.1 \times 10^{-6}\ \text{s} $

Determining Frequency Error

The error in the measured frequency ($\Delta f$) is related to the error in the measured period ($\Delta T$). We can approximate this relationship using calculus. If $f = 1/T$, then the change in $f$ ($\Delta f$) due to a change in $T$ ($\Delta T$) is given by:

$ \Delta f \approx \left| \frac{df}{dT} \right| \Delta T $

Calculate the derivative of $f$ with respect to $T$:

$ \frac{df}{dT} = \frac{d}{dT} (T^{-1}) = -T^{-2} = -\frac{1}{T^2} $

Now, substitute the values into the error approximation:

$ \Delta f \approx \frac{1}{T^2} \Delta T $

$ \Delta f \approx \frac{1}{(10 \times 10^{-6}\ \text{s})^2} \times (0.1 \times 10^{-6}\ \text{s}) $

$ \Delta f \approx \frac{1}{(10^{-5}\ \text{s})^2} \times (10^{-7}\ \text{s}) $

$ \Delta f \approx \frac{1}{10^{-10}\ \text{s}^2} \times 10^{-7}\ \text{s} $

$ \Delta f \approx 10^{10}\ \text{s}^{-2} \times 10^{-7}\ \text{s} = 10^3\ \text{s}^{-1} = 1000\ \text{Hz} $

Convert the error to kHz:

$ \Delta f \approx 1\ \text{kHz} $

The maximum error in the measured frequency is approximately 1 kHz.

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Important Questions from Error Analysis

  1. The measurement errors mainly caused by human mistakes are called-

  2. A tangent galvanometer is a:

  3. Null type recorders are __________ recorders.

  4. What is the smallest change in the input signal that can be detected by an instrument called?

  5. Errors that occur after taking care of all gross and systematic errors are called as:
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