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ECEN5633 Radar Theory Lecture #25 14 April 2015 Dr. George Scheets www.okstate.edu/elec-eng/scheets/ecen5633 n Read 5.3 n Problems 5.3, Web10 & 11 n Reworked.

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Presentation on theme: "ECEN5633 Radar Theory Lecture #25 14 April 2015 Dr. George Scheets www.okstate.edu/elec-eng/scheets/ecen5633 n Read 5.3 n Problems 5.3, Web10 & 11 n Reworked."— Presentation transcript:

1 ECEN5633 Radar Theory Lecture #25 14 April 2015 Dr. George Scheets www.okstate.edu/elec-eng/scheets/ecen5633 n Read 5.3 n Problems 5.3, Web10 & 11 n Reworked Exams u Due 16 April (Live) u Due 23 April (DL) n Quiz #3 u Live on 21 April u DL < 28 April

2 ECEN5633 Radar Theory Lecture #26 16 April 2015 Dr. George Scheets www.okstate.edu/elec-eng/scheets/ecen5633 n Read 5.5, 6.1 n Problems Web 12, 13, & 14 n Reworked Exams u Due 16 April (Live) u Due 23 April (DL) n Quiz #3 u Live on 21 April u DL < 28 April

3 h(t) Delays Low Frequency Output x(α) h(α) x(t-α)

4 Impulse Response h(t) h(t) Impulse In Matched Filter (FIR Filter) FIR weights = sampled values of h(t)

5 How does Chirping affect… n … the Ambiguity Function? n … a doppler shifted waveform? n … the P(Hit)? x(t) What you might see at: Direct Conversion Receiver Output of Mixer Low Pass Filter Up Chirp Local Oscillator tuned to f low Phases happen to match

6 Down Chirp Ambiguity Function

7 How does Chirping affect… n … the Ambiguity Function? u Tilts it x(t)

8 Chirp: No Doppler n Top: Matched Filter Output n Middle: Input n Bottom: Matched Filter Impulse Response n t p = 1 second n (Δf/2) *t 2 = 3t 2 (rate of phase change) Instantaneous Frequency = 6 Hz at t p seconds = Δf*t p at t p seconds

9 Chirp: 0.1 Hz Doppler n Top: Matched Filter Output n Middle: Input n Bottom: Matched Filter Impulse Response

10 Chirp: 1 Hz Doppler n Top: Matched Filter Output n Middle: Input n Bottom: Matched Filter Impulse Response

11 Chirp: 4 Hz Doppler n Top: Matched Filter Output n Middle: Input n Bottom: Matched Filter Impulse Response

12 Chirp Radar n Transmit a long pulse u Get range resolution of short pulse n Long pulse has > energy than short pulse n Can get by with lower voltages n Doppler Shift → Wrong range n Can get around this by… u Matching up chirp with down chirp

13 Down Chirp Ambiguity Function source: Levanon, Radar Principles

14 How does Chirping affect… n … the Ambiguity Function? u Tilts it n … a doppler shifted waveform? u MF peak is at wrong time Up Chirp

15 How does Chirping affect… n … the Ambiguity Function? u Tilts it n … a doppler shifted waveform? u MF peak is at wrong time n … the P(Hit)? x(t)

16 Some Equivalent E signals n 1 vp Square Pulse, t p = 1 microsecond Power = 1 watt, Energy = 1 μ joule n 2 0.5 vp sinusoid, t p = 1 microsecond Power = 1 watt, Energy = 1 μ joule n 2 vp Square Pulse, t p = 0.25 microsecond Power = 4 watt, Energy = 1 μ joule n 0.2 vp sinusoid, t p = 25 microsecond Power = 0.04 watts, Energy = 1 μ joule

17 Matched Filter Output SNR n SNR < 2E/No u = at optimum sample time & input signal is perfectly matched u SNR = 2P r t p /N o = P r /(N o W N ) [Baseband Pulse] u SNR does depend on W N F WN depends on pulse envelope shape n SNR does depend on T o sys n Considerable Flexibility for Pulse Shape u What matters is the Energy

18 Radar Equation n Yields RF power at antenna output n No Chirp? No doppler? Direct Conversion Receiver Baseband pulse (out of Mixer LP Filter) n Chirp? Time Varying Sinusoid n Sinusoid packs less energy n Do we need to adjust P(Hit) equations?

19 How does Chirping affect… n … the Ambiguity Function? n … a doppler shifted waveform? n … the P(Hit)? u Direct Conversion Receiver? u P r effectively takes a 3 dB hit

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