2011 2nd International Conference on Networking and Information Technology IPCSIT vol.17 (2011) © (2011) IACSIT Press, Singapore Additional Data Transmission in AM Broadcasting System Based on Very Minimum Chirp Keying Yajun Liu, Guoxin Zheng and Zhiyi Qiu School of Communication and Information Engineering, Shanghai University, Shanghai,200072,China e-mail:junerliu2003@163.com Abstract—This paper presents an AM broadcasting system based on in-band multiplexing, of which modulating carrier signal is VMCK(Very Minimum Chirp Keying) instead of sine wave in conventional AM systems. Multimedia data can be transmitted during broadcasting analog audio signal without extra band. The simulation shows that good performance of both modulations could be obtained under certain conditions. Keywords-UNB; VMCK modulation; AM 1. Introduction DSB-AM modulation is one of the oldest audio broadcasting modulations, which uses envelope detection to lead to a low cost of the receiver, also plague the low spectrum efficiency and vulnerable anti-interference performance. This kind of communication systems modulate the analog audio information with sine wave of which the frequencies range from Mega-Hz to hundreds Mega-Hz. From the perspective of frequency domain, it transfers the audio information in the range of 300Hz to 3400Hz to a higher frequency area. For one thing, it avoids the low frequency information to be interfered by the low frequency surrounding noise; in the other hand, it facilitates the signals to be sent in a small size. In the transmitting process, the sine wave doesn’t carry any information. It only expresses the audio information in the way of varying the amplitude of the wave. According to the relevant national standard, the audio bandwidth of analog AM broadcasting is excepted to be 50Hz to 5000Hz, and the voice bandwidth is from 300Hz to 3400Hz.Hence, form the point of receiving signal view, there is a total vacuum spectrum near the carrier ±50Hz or ±300Hz. In addition, if considering the dynamic performance of the different audio signal’s spectrum component and the breaks in the broadcasting process, the vacuum spectrum is to be wider in statistical significance [1]. How to use this vacuum spectrum of the DSB-AM modulation to transmit more information effectively is to be of great importance. VMCK modulation is one kind of the UNB (Ultra Narrow Band) modulation. Compared with the conventional modulation methods(FSK,ASK,PSK etc.), UNB modulation can transmit data in the same rate only use a fraction of or even one of a dozen bandwidth of the former, so it can raise the band efficiency dramatically. As one of the UNB modulation methods, VMCK has narrower spectrum, and the attenuation degree of the side lobe is better. As a result, in order to maximally its narrow band specialty, we propose to replace the sine wave by VMCK signal as the carrier. The additional data is transmitted on the basis of approximately the same spectrum of the original system without changing the DSB-AM system as well as not bring a significant impact on the analog audio transceiver performance. The mathematic analysis and simulation are carried out. The way of multiplex modulation makes use of valuable spectrum resource effectively and retains the broadcasting transmitted power the same. 2. AM-VMCK Modulation 173 2.1 VMCK modulation VMCK modulation represents logic “1” and “0” with the chirp frequency increase (up-chirp) and the chirp frequency decrease (down-chirp).The phase is continuous between any two adjacent signal waves, and it is characterized by its extremely narrow spectrum. Single circle VMCK signal V (t ) in a circle t ∈ [0, T ] express as: V1 (t ) = sin[2π f s (1 − α + α f s t )t ] (1) (2) V2 (t ) = sin[2π f s (1 + α − α f s t )t ] Here, s 1(t ) and s 2(t ) represent data 1 and 0 respectively, f s is the bit transmission rate, α( 0 < α < 1 ) is the chirp modulation factor which represents the change degree of the linear frequency. When α = 0 , they are both sine waves and, as the carrier, don’t carry the additional information. It is the same as the regular DSB-AM system. The more α increased, the more different between the two signals, and the wider the spectrum is. Particularly, V1 and V2 are orthogonal when α = 0.731 , and that is the best demodulation spot [5]. Figure1 are VMCK waveforms with different α. Waves of VMCK 1 V1,a=0.731 V2,a=0.731 V1,a=0.2 V2,a=0.2 0.8 0.6 0.4 Amplitude 0.2 0 -0.2 -0.4 -0.6 -0.8 -1 0 0.1 0.2 0.3 0.4 0.5 0.6 Normalized Time 0.7 0.8 0.9 1 Figure 1 . VMCK waveforms with different α 2.2 AM-VMCK system Figure2 shows the AM-VMCK compound modulation system. The analog audio, AM-DSB, modulation adopts VMCK signal as the carrier. Firstly, DC component is added to the audio signal to ensure the amplitudes of all signals are above zero. Here, the relative size of the DC component and the amplitude of the signals determine the signal’s modulation depth. Meanwhile, the added digital information is converted into binary data and then become a series of carriers after being modulated by the VMCK modulation. Secondly, these two modulated signals are multiplied and become multi-modulation signals, that is, the audio signal with low frequency is transferred to the signal’s center frequency f s . Lastly, after being filtered by BPF, the signal is sent out by the antenna. The receiving signal is demodulated in two ways. In one way, the signal is passed the BPF with the center frequency f s and then carried on envelope detection. After that the DC component is removed, the demodulated audio information is obtained. This is the original analog audio demodulation. In the other way, the demodulation takes the correlation operation using the up-chirp and down-chirp which have the same frequency with the transmitting signal, and then the result is compared and decided as binary data. In this way the additional digital information of the transmitting terminal can be recovered. 174 Figure 2 . System diaagram of the compound c moodulation The trannsmitting siggnal is: s (t ) = U c [1 + ka (t )]V (t ) (3) Here, a (t ) is the analog audioo signal, M is the DC level, V (t ) is the digiital signal modulated m byy VMCK moddulation. Noticing that there is no much difference between VMC CK signal annd sine wavee sin ωc t , so o V1 (t ) can bee separate intto an additioon of two paarts which are a sine wav ve and anothher wave c1 (t ) which is derived ass follows c1 (t ) = V1 (t ) − sin 2π f s t = sin[2π f s (1 − α + α f s t )t ] − sin 2π f s t (4) = −2 cos[2π f s t − πα f s (1 − f s t )t ]sinn[πα f s (1 − f s t )t ] That is: V1 (t ) = c1 (t ) + sin 2π f s t (5) c2 (t ) V2 (t ) can be deerived in the same way: c2 (t ) = 2cos[2π f st + πα f s (11 − f s t )t ] • sin[πα α f s (1 − f s t )t ] (6) V2 (t ) = c2 (t ) + sin 2π f s t (7) From (55)and (7) wee can see thaat c1 and c2 (as c (t ) ) are a the differrence of V1 aand V2 whiich representt ‘0’and ‘1’ separately s .T That means additional a diggital informaation is loadeed in c (t ) off which the frequency iss the same as the carrier’ss. In the VMCK modulattion, α , chirp p modulationn factor, reprresents the ch hange degreee of the lineaar frequencyy. With the increase of α , amplitud de of c ( t ) , which is thhe diversity of V (t ) andd T makes the t data moddulation easy. But the spectrum and transmitting power will bee sin(t ) , becomes lager. This needed morre at the sam me time and the demodullation of anaalog audio siignal will bee more interffered. So α should be coonsidered intto all factors.. Figure33 and Figuree4 are the waveforms w o V1 (t ) , c1 (t ) and sin(t ) , when α = of =0.1,0.4 and 0.731. Thee amplitude of o c1 (t ) in Figure3 F channges slowly, while w in Figu ure4 it changes fast. 175 a=0.1 1 c1(t) sin(t) V1(t) 0.8 0.6 0.4 0.2 0 -0.2 -0.4 -0.6 -0.8 -1 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Figure 3 . Comparison of three waves when α = 0.1 a=0.731 1.5 c1(t) sin(t) V1(t) 1 0.5 0 -0.5 -1 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Figure 4 . Comparison of three waves when α = 0.731 After passing through a AWGN (additive white Gaussian noise) channel the receiving signal is: r (t ) = U c [1 + ka (t )]V (t ) + n(t ) (8) n (t ) is additive noise , U c is the amplitude of carrier , k is the AM coefficient. As is shown in Figure2, the receiving signal is demodulated with two methods. One is to demodulate audio signal and the other is to demodulate the added data. The method of audio demodulation is DSB-AM demodulation by the BPF and envelope detection. Put (4),(5) or(6),(7) into (8), we can get: r (t ) = U c [1 + ka (t )](c(t ) + sin 2π f s t ) + n(t ) = U c c (t ) + U c ka (t )c (t ) + U c ka (t ) sin 2π f s t (9) + U c sin 2π f s t + n(t ) The Figure3 shows that, V (t ) is similar with sinusoidal carrier when α is small, and the frequency of c(t ) is the same with V (t ) ’s , which is f s . So after passing BPF and envelope detection, the result is: d (t ) = U c ka (t )c(t ) + U c ka (t ) + n′(t ) (10) n′(t ) is the baseband noise. For the digital data demodulation, we design the receiver according to the criterion that is the minimum error probability detecting signal with the noise’s interfere[6]. Suppose the two might be receiving signals are (a (t ) + M )V1 (t ) and (a (t ) + M )V2 (t ) , and the last time is T , the noise of input n(t ) is white Gaussian 176 noise of which the mean is zero and the unilateral power spectrum density is n0 , prior probability P (V1 ) = P (V2 ) . Comparing to the carrier, the envelope changes quite slowly, that is: U c [1 + ka (t )] = U c [1 + ka ] = a′ (i − 1)T ≤ t < iT (11) So, we suppose the amplitude of carrier stays the same in a T time. In the observe time (0, T ) , the observe wave y (t ) is expressed as: y (t ) = {( a′V1 (t ) or a′V2 (t )}+n(t) (12) For n (t ) is white Gaussian noise of which the mean is zero, and the probability density fV1 ( y) and fV2 ( y) are Gaussian distributions, so when: P (V1 ) exp{− 1 n0 T 0 [ y (t ) − V1 (t )]2 dt} > P (V2 ) exp{− 1 n0 T 0 (13) [ y (t ) − V2 (t )]2 dt} The receiving signal is decide to be V1 . For P (V1 ) = P (V2 ) , formula (14) can be simplified as: T 0 T y(t )V1 (t )dt > y(t )V2 (t )dt 0 (14) And vice versa, the receiving signal is decide to be V2 . This is the decision principle followed in this system. On the condition that the priori probabilities are equal, the bit error rate (BER) of any time point is: E (1 − ρ ) 1 Pe = [1 − erf [a′ b ]] 2 2n0 (15) Here, ρ is the correlation coefficient of V1 (t ) and V2 (t ) , erf ( x ) is error function, Eb is the power of V1 (t ) and V2 (t ) ( E1 = E2 = Eb ). To derive the system BER, the BER of every time point needed to be integrated. If a (t ) is sine wave, and ′ = (1 + k )U c , amin ′ = (1 − k )U c .For the probabilities of angle the modulation depth is k , then amax appearance are equal, when k is constant, the system BER is: Pesys = 2π 0 = 2π 0 f (θ ) p(θ )dθ 1 1 E (1 − ρ ) ]]dθ • [1 − erf [a′(t ) b 2π 2 2n0 (16) here, a′(t ) = U c (1 + k cos θ ) (17) 3. Simulation and Analysis The frequency of the carrier is at intermediate frequency in the simulation,441kHz, in order to meet for the entire AM band. The audio material is a fraction wav file My Chinese Heart. The random series of ‘0’and’1’ are modulated by VMCK, and then VMCK signal is further modulate the analog audio and VMCK signals with DSB-AM. The transmitting signal is shown in Figure5. Figure6 is the input and output SNR curves of the system when α is 0.1, 0.4 and 0.731.The output SNR means the SNR of the audio signal after the envelope detection. As is shown in the Figure, with the increase of α , the output SNR decreases, and the situation becomes worse by the increase of the input SNR. The three output SNR curves are alike when the input SNR is from 0dB to from 0dB to 10dB, after10 10dB the difference behaved differently .That is because the change of α impacts the demodulation. The smaller α is, the less VMCK wave and sine wave differ, so the audio transmission is better and the additional data transmission is worse. When α becomes larger and larger, the result goes into opposite. The reason is that the interference caused by the additional data accounts for more parts. 177 Figure7 is the BER curves with these different α .The Figure illustrated that BER deceases with the increase of α .When the input SNR is above 15dB, there is no error bit in α =0.731 and α =0.4 , and the BER is close to 10 −4 when α =0. 1. The modulated signal 2 1.5 1 0.5 0 -0.5 -1 -1.5 -2 0 0.5 1 1.5 2 Time 2.5 -3 x 10 Figure 5 . Waveform of the transmit signals 25 20 output SNR/dB 15 10 5 0 -5 -10 0 5 10 15 20 input SNR/dB 25 30 35 Figure 6 . Curve of input and output SNR 0 10 a=0.1 a=0.4 a=0.731 -1 BER 10 -2 10 -3 10 -4 10 -20 -15 -10 -5 0 5 input SNR/dB 10 15 20 25 Figure 7 . Bit error rate(BER)caves of the additional data 4. Conclusions The article proposes a band multiplexing method in AM broadcasting and simulates it with analysis. The simulation demonstrate that when the input SNR is small, the change of α plays a slight effort on the output SNR but has a serious effort on the BER performance, so a large α should be chosen at this time; When the input SNR is fairly large, the change of BER counts less with different α input, but significantly affect output SNR, so a small α should be adopted. A 44.1kbps additional data rate is obtained from the simulation, which could be used to transmit words, pictures or even H.264 video. 5. References 178 [1] Chenhao qi,Lenan wu. 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