To estimate the integration time required to detect Cassiopeia A at 1420 MHz using a 1-meter dish, we need to consider the signal-to-noise ratio (SNR) and radiometer equation. Here's a breakdown:
Flux Density of Cas A at 1420 MHz:
Cas A is decreasing in brightness over time, but as of recent measurements:
Dish Diameter: 1 meter
Effective area (assuming efficiency ~70%):
System Temperature:
At L-band, T_sys ≈ 100 K is typical for amateur setups (depends on LNA, environment, etc.)
Bandwidth:
Let's assume a moderate bandwidth of 1 MHz for neutral hydrogen work.
Radiometer Equation:
SNR=Sν⋅Aeffk⋅Tsys⋅2⋅Δν⋅t\text{SNR} = \frac{S_\nu \cdot A_{\text{eff}}}{k \cdot T_{\text{sys}}} \cdot \sqrt{2 \cdot \Delta \nu \cdot t}where:
kk is Boltzmann’s constant =1.38×10−23= 1.38 \times 10^{-23}
tt is integration time in seconds
We rearrange to solve for tt when a detectable SNR ~5 is desired:
Plugging in values:
Sν=1500×10−26S_\nu = 1500 \times 10^{-26}
Aeff=0.55A_{\text{eff}} = 0.55
Tsys=100T_{\text{sys}} = 100
Δν=1×106\Delta\nu = 1 \times 10^6
SNR=5SNR = 5
Let’s correct units and simplify numerically:
Approximately 0.35 seconds of integration time would be enough to detect Cas A at 5σ using a 1-meter dish with a 1 MHz bandwidth, assuming system temperature ~100 K and decent LNA.
This is an ideal estimate.
In practice, interference, system noise variations, and calibration errors will require longer integration, typically:
1–10 minutes to clearly distinguish the signal in drift scan or total power mode.
Cas A is also resolved out by some small dishes—beamwidth should encompass the full source.

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