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Mixer Spur Calculator

Calculate mixer spurious products (m×fLO ± n×fRF) for superheterodyne receiver design. Identify problematic spurs near the IF passband and optimize LO/IF frequency planning.

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Formula

fspur=mfLO±nfRF,m+nNf_{spur} = m \cdot f_{LO} \pm n \cdot f_{RF}, \quad m+n \leq N
fRFRF input frequency (MHz)
fLOLocal oscillator frequency (MHz)
mLO harmonic order
nRF harmonic order
NMaximum spur order (m+n)
fIFIntermediate frequency (MHz)

How It Works

In a superheterodyne receiver, the mixer multiplies the incoming RF signal with a local oscillator (LO) to produce an intermediate frequency (IF). The ideal mixer output contains only fLO - fRF (the desired IF) and fLO + fRF (which is filtered out). However, real mixers are nonlinear devices, and their transfer characteristics generate harmonics of both the LO and RF signals. These harmonics interact to produce spurious outputs at every frequency m*fLO +/- n*fRF, where m and n are non-negative integers. The total order of a spur is defined as m + n. Lower-order spurs (m + n <= 3) are typically the strongest and most problematic because higher-order products decrease roughly as the (m+n)th power of the input signal level. However, the rate of decrease depends on the mixer topology and drive levels. The image frequency is one of the most critical spurious responses. For a receiver with fLO > fRF (high-side injection), the image frequency is fimage = fLO + fIF, which corresponds to the 1x1 spur (m=1, n=1) at fLO + fRF. Any signal at the image frequency will be down-converted to the same IF as the desired signal and cannot be distinguished after mixing. This is why image-reject filters or image-reject mixer architectures (such as Hartley or Weaver) are essential in superheterodyne design. A spur chart is a systematic tool for evaluating all spurious products across a range of RF and LO frequencies. By plotting m*fLO +/- n*fRF lines on a frequency chart, the designer can identify which spur products fall within or near the IF passband. The goal of frequency planning is to choose LO and IF frequencies such that no significant spur products overlap with the desired IF band. Double-balanced mixers suppress even-order LO and RF products (even m or even n), significantly reducing the number of problematic spurs compared to single-ended or single-balanced topologies. A double-balanced mixer ideally passes only products where both m and n are odd. In practice, finite balance means some even-order leakage occurs, but at reduced levels (typically 20-40 dB below odd-order products). When selecting an IF frequency, the designer must balance several competing requirements. A higher IF provides better image rejection (the image is further from the desired signal and easier to filter), but higher-order spurs become more densely packed near the IF. A lower IF simplifies the IF filter design but brings the image frequency closer to the desired RF, making image rejection harder. In many modern receivers, a double-conversion or triple-conversion architecture is used to address these trade-offs, converting first to a high IF for image rejection, then to a lower IF for channel selectivity.

Worked Example

Given fRF = 915 MHz and fLO = 1060 MHz, the desired IF is |1060 - 915| = 145 MHz. The image frequency is fLO + fIF = 1205 MHz. Third-order spurs: 2x1060 - 915 = 1205 MHz (image!), 2x915 - 1060 = 770 MHz. The 2xLO-RF spur at 1205 MHz coincides with the image -- this receiver needs an image-reject filter or different IF selection.

Practical Tips

  • Choose IF frequency to minimize overlap between spur products and the desired IF band
  • Use the spur chart to compare high-side vs low-side LO injection -- one usually has fewer problematic spurs
  • Lower-order spurs (m+n <= 3) are strongest and most critical to avoid
  • Consider a double-conversion architecture if no single IF avoids all critical spurs
  • Double-balanced mixers suppress even-order products, reducing the total number of significant spurs
  • Always check the image frequency first -- it is the single most important spurious response in any superheterodyne receiver

Common Mistakes

  • Ignoring the image frequency (fLO + fIF for low-side injection, fLO - fIF for high-side)
  • Not checking even-order spurs in single-ended (unbalanced) mixer topologies
  • Assuming higher-order products are always negligible -- at high drive levels, 5th-order spurs can be problematic
  • Forgetting that LO harmonics interact with RF harmonics to create additional spur products
  • Choosing an IF that avoids low-order spurs but places a high-order spur directly in the IF passband at high input power levels

Frequently Asked Questions

A mixer spur is an unwanted output frequency produced by the nonlinear mixing process. Any mixer generates products at m*fLO +/- n*fRF for all integer combinations of m and n. Most of these are filtered out, but some may fall within the receiver's IF passband and degrade performance.
A spur chart plots all m*fLO +/- n*fRF products as lines on a frequency axis. The desired IF is highlighted. Any spur line that crosses or falls near the IF band represents a potential interference source that must be filtered or avoided by choosing different LO/IF frequencies.
The image frequency is an unwanted input frequency that produces the same IF as the desired signal. For low-side LO injection (fLO < fRF), the image is at fRF - 2*fIF. For high-side injection (fLO > fRF), the image is at fRF + 2*fIF. Image rejection is critical in superheterodyne receiver design.
In balanced (double-balanced) mixers, even-order products (m+n = 2, 4, 6...) are suppressed by the balanced topology. Odd-order products pass through. However, in single-ended mixers, all orders are present. The spur level generally decreases with increasing order, but the rate depends on the mixer's compression characteristics.

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