Physical Science Daily (2014) 154103 Acta Phys. Sin. Vol. 63, No. 15 Experimental study of microwave resonator tuning system* Pinnacle Yang Juan† Tang Mingjie Luoli Tao Wang and right (Astronautics, Northwestern Polytechnical University,Xi'an710072) (2014Year1Month9Date of receipt; 2014Year3Month18Date of receipt of revised) Round table resonant cavity and microwave generation and transmission apparatus and the outside world may form a separate microwave resonator system.Since the pressure difference on the wall of electromagnetic effects,Round table cavity may produce a net electromagnetic force,This need to give proof from the experiment.To this end the first response to a separate system into the microwave resonator Experimental study on-line tuning,The system time is in the resonant state,It is important to ensure that the net proved the existence of electromagnetic force.To this end,In this paper, round table resonator tuned for low-signal test,In conjunction with the tuning element,Accurate debugging2.45 GHz Resonant state frequencies,Influence of temperature on the resonant state analysis.Experimental results show that the resonant frequency of the microwave resonator2.44895 GHz, Quality factor117495.0823,And when the cavity wall temperature rise The resonant frequency is reduced, the quality factor to periodic oscillations. Key words: Apply electromagnetism, electromagnetic transmission, microwave radio equipment and facilities PACS:41.20.-q, 41.20.Jb, 07.57.-c DOI: 10.7498 / aps.63.154103 1 Lead Speech Free space using electromagnetic pressure generating electromagnetic form Thrust has been confirmed by research papers published [1,2], Which generates thrust system is an open system relatively free space, if the microwave resonator system electromagnetic pressure difference can generate an electromagnetic force, would give rise to a new type of the propulsion program. Microwave resonator system consists of a round table and a microwave resonant cavity production Health and transport equipment, of which the resonator round table is the main source of net electromagnetic force. Round table resonator made of a metal conductor, if the electromagnetic resonance phenomenon is input to the cavity, the body in any position of the reflected wave and the phase of the incident chamber are equal, the total electric field and magnetic field amplitude is superimposed directly incident and reflected waves, thus the total electric and magnetic fields, respectively, greater than the amplitude of the incident wave amplitude. then appropriately selected resonant mode, so that the front and rear ends of the wall surface of the cavity produce electromagnetic pressure difference, resonator will produce a net electromagnetic force distribution in the axial direction. increase the pressure difference exists and electromagnetic field amplitudes cavity resonator round table will produce a net 154103-1 Physical Science Daily (2014) electromagnetic force [3-5]154103 . Acta Phys. Sin. To prove a round table resonator net electromagnetic force experimentally the existence of In need of an external independent and microwave resonator system Vol. 63, No. 15 Experimental Research tuning, so that the system always in resonance. In this paper, a round table of low signal tuned resonator experiments, in conjunction with the tuning element accurately debug the state of 2.45 GHz resonance frequency, and experimental analysis of temperature on the resonant state the impact of the system parameters are given power characteristics in real conditions. 2 microwave resonator consisting of Round table by the microwave resonator cavity formed system is shown1 Shown, it is a precise frequency tracking system, made of iron Lithium battery conditioning power, signal source, amplifiers, waveguides, round table resonant cavity detector and radiator, of which the signal source and amplification When constituted solid source system to work, the signal is converted to electrical energy source Milliwatt, in 2.45 GHz electromagnetic energy input to the amplifier The amplifier in the power of action to milliwatts to hundreds of watts of energy amplification energy along the waveguide transmission to a round table resonant cavity. When the frequency of natural resonant frequency and the signal source output of round table is the same resonator, the electromagnetic wave in a round table resonant cavity resonator, a detector signal is maximum value of the state, a round table may have an axial cavity net electromagnetic force F. On the contrary, when a round table and a cavity resonance frequency signal source output frequency is not at the same time, the detector signal is at a very low level, Then continue to change *National Natural Science Foundation of China(Approval number: 90716019)Project supported by. †Corresponding Author. E-mail: yangjuan@nwpu.edu.cn ©2014 Chinese Physical SocietyChinese Physical Society 154103-2 http://wulixb.iphy.ac.cn Physical Science Daily (2014) 154103 Acta Phys. Sin. Variable output frequency signal source, and a round table until the cavity resonance frequency coincide, then the detector signal reaches the maximum value, the electromagnetic resonator system resonance, round table cavity may produce a net electromagnetic force. Literature [6] Theoretically discussed the resonator quality factor and net electromagnetic force is proportional to the round table, and thus accurate resonant cavity and having a high quality factor is a key factor in a net electromagnetic force at its resonant frequency. ړԼ ܸ ܸ ᑿ ܸ ܸ가 ԍܸ ฉ 8 Ԧܸ ฉ Кܸ ฉ F ฉ ܸ 8ܸ ஊ ܸܸ ႃ ܸ ܸ ܸܸ ܸ ηՂܸ Drawing1Microwave resonator system structure diagram Vol. 63, No. 15 Taiwan cavity resonance at 2.45 GHz in the TE011 mode. 3.2 Match guarantee system based on conditions For the FIG.1 Microwave resonator system shown, a round table resonance Cavity waveguides and three solid source equivalent impedance equal system of To match, this time completely absorbed microwave power resonator [ 8]. When the system does not match the power output of the microwave cavity with a reflective, Then need to generate a cavity near the new reflected wave, it just reflected wave amplitude and phase, cancel each other, so as to achieve the system match. Produces a reflected wave of this new approach is to use a rectangular microwave coupling window and double spiral As shown dispenser2 , In which a rectangular window with a microwave Ԧܸη Ղ coupling between the resonator and waveguide circular table, double spiral ᣣ deployment is used in a microwave coupling ࠱ ܸ between the rectangular windows and solid ܸܸ 8 source. Adjust the appropriate rectangular micro ڍগ ܸ Wave coupling window sizeL1,L2 And twin screw dispenser two screws Depth L3,L4It can make the microwave resonator system to achieve accurateMatching state. oscillation frequency of the applied power frequency ω and ω0 RLC circuit coincides, resonance, electromagnetic energy is the largest closed waveguide cavity resonance circuit in principle stored and the same, and thus the resonance condition occurs as follows: 1) cavity 3 Guarantee microwave resonator system resonant state Condition 3.1 Based resonator structure to ensure that the conditions of Electromagnetic waves transmitted into the waveguide cavity closed period, both energy storage field, can store magnetic energy, which cavity can be equivalent to a low-frequency RLC circuit. When the free The maximum power and maximum (energy ) 1 n equal;2) the presence of the cavity + 4 2 154103-3 Physical Science Daily (2014) 154103 ԥ ᛃ ܸ Acta Phys. Sin. Vol. 63, No. 15 Drawing2Microwave resonator matching components(A) Rectangular microwave coupling window; (B) Twin-screw dispenser ܸ8 L 4 Low Signal frustum cavity L L debugging L 4.1 Debugging principle (A) (B) ) Or (1 n Pure standing wave,n= 1, 2, 3·; 2 + 2 3)Cavity Equal to the inductance and capacitance of anti-anti.Theoretically, microwave resonant cavity resonance Vibration mode significantly in has order diversified to generate an electromagnetic force needed In the round table to select the equivalent resonant cavity, high quality factor TE011 Mode. A microwave theory [7],TE011It can only exist in a cylindrical mold Resonant cavity. And for the round resonator,TE011Electromagnetic table special mold Zheng equation can not be solved. But if a round table cavity side wall mining TE01 microwave mode coupling rectangular will excite waveguide resonant cavity in a round table similar cylindrical resonator mode of the electromagnetic field ᅾ ॎ ฉ In the resonant mode and the resonant frequency determined conditions, according to the resonance Cavity theory, we can design and processing of the round table resonant cavity. In fact, Because of the design calculations, fabrication and assembly errors that could cause actual cavity Offset from the ideal resonant structure; ambient temperature changes and another cavity surface skin depth heat effect on the radial and axial dimensions of the cavity can also lead to changes, these uncertainties affect not only the resonant frequency of the resonant cavity, also affects the quality of factor. and thus to determine the specific structure of the cavity resonance frequency and quality factor resonator according to a debugging test method return loss. Return loss is defined as Pr distribution TE011, TE011 and therefore is used here to describe the use of a resonant mode. A microwave resonant cavity theory, literature [6] To determine the electromagnetic resonator Structure system frustum cavity, thereby theoretically guarantees round Lr= 10 lg 154103-4 P1 , (1) Physical Science Daily (2014) 154103 Acta Phys. Sin. Among themPrReflected from the cavity of power,P1As an input to the harmonic Power oscillator cavity definition quality factor Q of the total storage resonant cavity electromagnetic field within a period 2π times the energy loss ratio, that is, W ω0 W Vol. 63, No. 15 Before, the first network analyzer short calibration, which reflectance measurements are normalized. Debugging device and then connected standby, measurement resonant in resonant frequency, return cavity quality loss near the factor is determined by the size of the replacement cap, rectangular microwave Coupled windows and Q=2π p LT 0 = , (2) pL Among themWIntraluminal electrical, magnetic total energy storage,pLThe average loss for the resonatorPower consumption,T0Resonance cycle. Drawing3 Shows a typical return loss test curve,Curve the deployment of Lr min Lmin f1f0f2 Drawing3Return Loss test curve analyzer via microwave transmission cable resonator connection. Debugging ࠱ܸ ᄦ ܸ ᑿ twin screw adjustment screws deep Degree adjustmentTest, To determine the resonance at 2.45 GHz, with the highest Structural combination of merit. The lowest point of the resonant state, a frequency corresponding to the resonance frequency f0. Quality factor according to To calculate,Its f0 f0 the formulaQ= = f2-f1 Δf InΔf=f2-f1Resonance frequency bandwidth.Visible,Resonant frequency The ratio of the resonant frequency bandwidth determines the quality factor. As shown4 , The microwave resonator tuning system consists of a network analyzer, the rectangular microwave coupling window, double spiral dispenser and round table resonator consisting of a round table and the side wall cavity size cap structure, in which the network ړ Լ ܸ a ԥ ܸ ܸ ܸ8 Տܸ ܸ ࠱ܸ ܸ Я ܸ ງ ए Οܞ ࠱ܸ ܸ Я ܸ ງ ए ܸܸѬܸ 가 ܸܸ ܸ ܸ Ռ ܸ ࠱ܸ ᄦ 154103-5 Physical Science Daily (2014) 154103 Acta Phys. Sin. Vol. 63, No. 15 Drawing4Microwave resonator tuning system 4.2 Commissioning results and analysis 4.2.1. Debugging round table resonator 1) cover a combination of different sizes. With 7 sets of different size cap retraction depth, you can get 49 kinds of different combinations of retraction for the size of the end surface at different depths, choose the large end after commissioning retraction depth 4 mm, small end face retraction depth 12 mm for the best combination, then the resonant frequency closest to 2.45 GHz, and the quality factor most High its return loss curve is shown5 (A), the draw resonance frequency of 2.4500 GHz, resonant bandwidth of 2.5×10-3GHz, quality Factor 976.9753. 2) The rectangular structure of different microwave coupling window. Adopted 15 different sizes of rectangular microwave coupling window, in the best combination of size, based on the end cap, through commissioning, and ultimately selectedL1= 43.34 mm, L2= 31.78 mm rectangular microwave coupling window of the best, then the resonant frequency closest to 2.45 GHz, and the highest quality factor. Its return loss curve is shown 5 (B), the draw resonance frequency 2.4500 GHz, resonant bandwidth of 1.6×10-3GHz, quality factor 1512.887. 4.2.2 And the double helical structure of the deployment of the best round table resonator debugging Based on the above circular table in the debug resonator, the increase in twin screw dispenser for debugging, adjust double screw insertion depth until the best results are shown debug5 (C), the resonance frequency at this time is closest to 2.45 GHz, and the highest quality factor. Draw resonance frequency 2.44895 GHz, resonant bandwidth of 2.0843×105 GHz, quality Factor of 1.175 × 105. 154103-6 Physical Science Daily (2014) 154103 Acta Phys. Sin. Vol. 63, No. 15 0 -1.0 -2.0 Lr/dB Lr/dB -4 -3.0 -4.0 -8 -12 (A ) 2.44 f0= 2.4500 GHz Df= 2.5T10-3 GHz 2.45 2.46 2.47 (B -16) 2.43 2.44 f/ GHz f0=2.45 G H z Df= 1.6843T10-3 GHz 2.45 2.46 2.47 f/ GHz 0 Lr/dB -10 -20 -30 (C ) 2.4484 -40 f0=2.44895 G H z Df= 2.0843T10-5 GHz 2.4488 2.4492 2.4496 f/ GHz Drawing5Return Loss test curve(A)Optimal size end combinations; (B)Best of rectangular microwave coupling window; (C)Best screw depth twin screw dispenser 4.3 Effect of temperature on the cavity resonance condition 4.3.1 Experiment law According Return Loss test curve shows that the higher the quality factor, The narrower the resonance bandwidth and resonant frequency and quality factor more sensitive to deformation of the cavity. For this reason a heating source in the outer wall of the cavity to produce the effect of thermal deformation of the cavity structure. The heat source were placed small endFace, big face and the side wall surface, Measure The amount of return loss, and then determine the resonant frequencyf0And a minimum return lossLrmWith the heat source temperature changes as shown in6 Figure6 (A), (b) As a heat source placed small end test results show that the temperature shown from32.5 Between oscillation and the amplitude basically unchanged from FIG.6 Also calculate Publisher The quality factor, the results show that the heat source is placed in different locations, the highest Quality factor are 120,000, the lowest quality factor are 40,000. 4.3.2 Analysis of experimental phenomena Resonant frequency falling This phenomenon can be a microwave cavity The perturbation theory [8]From electromagnetic theory to explain when the cavity wall by the perturbation, the following relationship: ω-ω0 (we-wm )·Δv ω0 = W ◦ , (3) CWhen raised to 49.9 ◦C, the resonant frequency is reduced from 2.4495 GHz to 2.44885 GHz, minimum return loss between -54 and -17 dB oscillation, and 154103-7 Physical Science Daily Acta Phys. Sin. Vol. 63, No. 15 154103 decreases. oscillation (2014) amplitude Where, ω is the the Figure6 (C), (d) a heat Source placed large end outer test results show that the temperature shown from29.5 ◦ C rises to40.4◦CWhen the resonance frequency reduction from 2.44970 GHz Small to2.449375 GHz, minimum return loss43 and-17 oscillates between dB, and the amplitude and then decreased. Figure 6 (E), (f) as a heat source placed outside the wall test results show that the temperature shown from 28.7 ◦ C rises to32.8◦CWhen the resonance frequency reduction from 2.44935 GHzSmall to 2.44915 GHz, minimum return loss at -42 and -17 dB resonant frequency perturbation round after; ω0 is the resonant frequency perturbation round before; we, wm were average power density and the magnetic energy density perturbations at; Δv to volume changes, when the cavity wall when concave , Δv <0, when the wall-convex, Δv> 0;. W after total average resonant cavity perturbation electromagnetic energy table1 It explained the situation of various disturbances varying frequency. Table1Wall-perturbation frequency changes Perturbation nature Perturbation region Strong magnetic field, a weak electric field A weak magnetic field, strong electric field 154103-8 Private perturbation Outbound perturbation Δv <0 Δv>0 ω> ω0ω <ω0 ω <ω0ω > ω0 Acta Phys. Sin. Physical Science Daily (2014) 154103 2.4495 Fifte -20 en 2.4494 -25 2.4493 -30 2.4492 -35 Lrm/ DB f 0/ GHz 2.4496 Vol. 63, No. 15 2.4491 -40 2.4490 -forty Five -50 2.4489 (A ) 32 34 36 3,840,424,446,485,052 2.4488 T/C T/C 2.44970 Fifte en -20 2.44965 -25 2.44960 -30 2.44955 -35 2.44950 -40 2.44945 -forty Five -50 -55 Lrm/ DB f 0/ GHz 2.44975 2.44940 2.44935 (C ) 28 30 32 34 36 38 40 (D ) 28 30 32 T/C 34 36 38 40 42 T/C -Fifteen 2.44935 -20 2.44930 -25 f 0/ GHz 2.44940 Lrm/ DB -30 2.44925 -35 2.44920 2.44915 (B ) -55 32 34 36 3,840,424,446,485,052 -40 (F) (E) 28 29 30 31 32 33 -forty Five 28 29 30 31 34 T/C 32 33 34 T/C Drawing6Measurement system resonant frequency and a minimum return loss varies with temperature (A), (b)The outer wall of the heat source placed small end; (C), (d)The outer wall of the heat source placed in the large end face; (E), (f)Placed on the side of the outer wall of the heat source resonant field, a weak electric field perturbation at the cavity electromagnetic field distribution outward. The above table shows that, after the [3]Found resonant According that to in round the table cavity inner wall surface of the cavity is always lower than frequency perturbation less than the resonant frequency perturbation ago. the average electric field strength and Return loss is a phenomenon of alternating magnetic field strength is always higher size network analyzer Scanning frequency can not than the average of the cavity in the be continuously caused, the network analyzer cavity normal working hours, the skin depth can heat loss within the cavity so that thermal frequency points.Drawing7 (A) shows the actual return loss curve, assuming two adjacent frequency points isf1,f2. deformation, In bolted thermal expansion that the wall being outwardly convex, this volume change is very small. In summary, this condition belong in a strong magnetic 154103-9 only give Return loss value scanning Physical Science Daily (2014) 154103 Acta Phys. Sin. With increasing heating time, the round table cavity volume continues to expand, Then t1,t2,t3And t4, the actual return loss curve gradually shifted to the left, the resonant frequencies of f1, f01, f02, f2, the lowest returnWave loss values areLminHowever, due to the network analyzer scanning frequency is unable to continue, the return loss curve and the actual curve recording can not be consistent, that is, when the return loss curve locatedf1And between f2, recorded the curve the distortion, scanning actually presence only frequency give of letter pointInterest Figure7 (B) gives the network analyzer return loss curve recording, scanning frequency interval Δf=f1- f2DefinitionLrif1,Lrif2Heating for a time at the actual curve i at a frequency return of loss f1, and return loss, minimum value when the value of f2, where i = 1, 2, 3, 4. forAt time t1, the network analyzer records real curve, the resonant frequency 15410310 Vol. 63, No. 15 Acta Phys. Sin. Physical Science Daily (2014) 154103 Vol. 63, No. 15 Ratef1,Minimum return lossLr1f2.Fort2Time,The internetTest curve distortion analyzer record,That test is still resonant frequencyf1,Insteadf01,Minimum Return Loss valuesLr2f2. The actual minimum return loss should For the time t3, the test curve network analyzer record resonant frequency Tof2,Insteadf02,Minimum Return Loss valuesLr3f1. Gradually increased -38 dB; when the heat For the moment t4, network analyzer records real curve, the resonant frequency f2, the minimum return loss Lr4f 1. Thus, due to the presence of sweep frequency interval, only on the scan frequencies only return loss measurement curve realistic, in addition to measurement curve distortion are present, it should be removed. Thus FIG.6 (B), (d) and (f) given by When, from -42 dB return loss down to -53 dB and then increased to be addressed as shown in curve8 Shown Curve. From Fig.8 Available, when the heat source is placed small end, the return loss source is placed large end from -53 dB to Lr -About 44 dB; when the heat source placed in the side walls, the return loss oscillation changes, but remain at -40 dB or less. Thus available, influence resonator quality factor reduction (return loss increases), the main factor is the small end temperature. Lr Lr1f1 Lr1f1 Lr4f2 Lr3f2 Lr2f1 t t t t D t4>t3>t2>t1 f t4>t3>t2>t1 (A ) f t t D f Lr1f2 Lr4f1 t f f t Lr2f2 Lr3f1 Lr1f2 Lr4f1 Lr3f2 Lr2f1 Lr2f2 Lr3f1 Lr4f2 f (B ) f f Drawing7Return loss curve(A) Actual curve; (B)Network analyzer sweep display curve -40 -38 -44 Lrm/ DB Lrm/ DB -42 -46 -48 -50 -52 (B) (A) -54 36 40 44 48 52 28 32 36 T⊳C T⊳C -39.5 -40.5 Lrm/ DB 32 -56 15410311 (C) 40 Physical Science Daily (2014) 154103 -41.5 Acta Phys. Sin. Vol. 63, No. 15 -42.5 28 29 30 31 32 33 T⊳C Drawing8The actual minimum return loss variation with temperature(A) Small end; (B) Large end; (C) Sidewall 15410312 Physical Science Daily (2014) 154103 Acta Phys. Sin. Powered amplifier, and constantly adjust the output frequency of the signal source to make the detector signal and keep the maximum, then the system resonance. Reference frustum cavity low signal results can be predicted in the actual power conditions the wall set frustum cavity skin depth of the microwave heating caused cavity expansion will make the system detuned, so that a detection signal decreases, and therefore actual power conditions of the system Debugging should be a signal to the resonant state detector marked the largest system after the system is powered on, the source first output center frequency 2.45 GHz, and then discovered that the detection signal is decreasing. After so the system is turned on, the signal source output frequency should be the center frequency began reduced in order to obtain the maximum value of the detection signal, down-step experiment is 10 kHz. 5 Microwave resonator system debugging under conditions of actual power 5.1 Debugging process Drawing9 Microwave resonator system under real conditions of power,Wherein lithium iron conditioning power on and off, solid source of switch and frequency by infrared remote control, and there is solid source monitor output and reflected power indicator on the power lithium iron conditioning system operation as follows: Open iron lithium battery conditioning supply, respectively, to the signal source and discharge ႃ ԍ ᛫ V ฉ 8 ԥ ᛃ ܸ8 Vol. 63, No. 15 ᥑ ܸ ڍগ ܸ ଊ ᧫ η Ղ ܸ ᥑ ҫ ႃ ႃ ܸ ҄ᄤ 8ܸ ஊ ᅾॎ ॲ Ռܸ ฉ ړԼ ܸ ᑿ ႃ ܸ ܸܸ ܸ ඵ шԂ8 Drawing9Microwave resonator system debugging power under real conditions 5.2 cavity detuning detector Debugging results 5.2.1 Resonant state detection 2.0 U= 0.8 Umax gives system Drawing10 Under the true ᣥѣ ဋ ܸ ဋ ᄱ power source output frequency Seen from ܸ the figure and the measurement curve detection signal voltage relationship,After power source output ᣥѣ ဋ frequency 2.45 GHz unchanged, due to the ଌ ܸ ဋ heat cavity resonance frequency decreasing, 15410313 ᣥѣ Physical Science Daily (2014) 154103 Acta Phys. Sin. detection signal U "0.8Umax resonance when the system is in good condition. Therefore, the actual down, the need to ensure the detector signal is always at 1.7 V or more. The feedback signal is decreasing. After quickly reduce output frequency signal source Rate, the output frequency is constantly approaching the resonant frequency resonant cavity tends, so the detector rising feedback signal. When the signal source output frequency substantially equal to the resonant frequency, the resonant cavity is in good condition, the feedback signal detector tends to be a great value. here believe a U/V 1.6 0.8 0.4 0 5.2.2 cavity surface temperature change In the real power, the thermal effect causes the temperature of the cavity wall cavity within the skin depth increases, so the study of the cavity surface temperature ဋ ܸ ܸ ဋ 1.2 2.4492 2.4494 2.4496 2.4498 Vol. 63, No. 15 2.4500 f/ GHz Drawing10 Relationship between the signal source and the detector output signal frequency between 15410314 Variation help verify whether the microwave resonator resonance shape State. To this end, we measured with a thermocouple as shown11 Cavity surface shown The surface temperature at different locations. Temperature measurement process should continue Reduce the output frequency of the signal source to ensure that the detector signal and keep The maximum value2.1 V at that time to ensure that the resonator is resonated measurement point temperature change over time as shown12 As shown in diagram indicating that the temperature at the center of the small end first began to rapidly rise, followed by temperature measurement points at other positions are also beginning to heat up, and the temperature close to each other, it was obvious that the end face of the center as a heat source. Acta Phys. Sin. Physical Science Daily (2014) 154103 Vol. 63, No. 15 D 6 Knot Theory D⊳ H D⊳ D Drawing11 Measurement point position 70 ࠱ܸ ᭧1ܫພए ࠱ܸ ᭧2ܫພए Ο ܞ3ܫພए 60 T/C 50 40 Ο ܞ4ܫພए ܸܸ ᭧5ܫພए ܸܸ ᭧6ܫພए 30 20 0 20 40 60 80 100 t/ S Drawing12 Cavity surface temperature change with time To explain the temperature variation, the first to be interpreted according to the theory of electromagnetic wave propagation equation round table resonant cavity. In order to obtain the maximum electromagnetic thruster force, requiring electromagnetic waves to the small end cutoff at a transmission, Deadline round the table wavelength √ resonator close On 2 In this paper, the rectangular waveguide transmission line, coupled windows and double screw adjustment Adapter to match the element, use a network analyzer to round table resonant cavity microwave resonator system conducted experiments debugging, and get the ideal resonant state that the resonant frequency of 2.44895 GHz, the quality factor of up to 117,000, and find the resonant frequency with the cavity continue to lower the temperature increases and return loss periodic oscillation experiment phenomenon from the working characteristics of the network analyzer sweep starting, explain the reasons echo oscillations and eliminate distortion return loss. For solid source of microwave resonator systems to large end wall cavity detector signal is a feedback signal, in real power conditions, the infrared remote control device to match the source remote switch and down after frequency detector signal remains the largest state in about 2.1 V, to achieve a precise tuning of the entire microwave resonator system, so that it can always be in resonance. Finally, the major point of the cavity wall temperature monitoring indicates small end cavity at the center of the heat the most significant, in line with the resonator characteristics of the work. The experiment It laid a good foundation for further independent microwave resonator system thrust measurement and dynamic experiments. Reference Wavelengthλ=λc,Group 1-(λ/λc) = 0.And velocityvg=c In the large end of the required wavelength of electromagnetic waves to free-space wavelength √ λ=λ0,Group velocityvg=c 1-(λ0/λc)2.This 15410315 [1] Geo ff rey A. Landis 2000 Microwave Pushed Interstellar Sail: Starwisp Revisited, AIAA3337 [2] Nakagawa T, Mihara Y, Komurasaki K, Takahashi K, indicates that electromagnetic Wave energy transfer to small end when all deposited onto the metal surface from Physical Science Daily Acta Phys. Sin. Vol. 63, No. 15 (2014) 154103 Sakamoto K, Imai T2004J. Spacecraft and Rockets41 Converted into heat within the skin depth of the end face, while at the end face of the large group velocity of electromagnetic waves near the speed of light, all the electromagnetic energy is reflected back to the wall, so that in the ideal case, the electromagnetic energy is not converted to the skin depth of the inner wall surface Thermal Round table resonant cavity electromagnetic field numerical results from existing microwave thruster view [3],Calcd electromagnetic field strength in the vicinity of the axis of the larger, which have demonstrated the higher the skin depth at the center of the end face of the small heat, thus heating up rapidly, and the temperature is higher than other locations. In theory, the large end surface skin Although not within the depth of the electromagnetic energy deposition, but with the extension of working hours thruster, since the metal heat conduction large end of the temperature will gradually rise. 15410316 151 [3] Yang J, Li P F, Yang L2011Acta Phys. Sin.60124101 (In Chinese) [Yang Juan,Lee Peng Fei,Yang Le2011 Physical Science Daily60124101] [4] Yang J, Wang YQ, Ma YJ, Li PF, Yang L, Wang Y, He G Q 2013 Chin. Phys. B Twenty two 050301 [5] Yang J, Yang L, Zhu Y 2010 J. Northwestern Polytechnic University28 807 (in Chinese) [Yang Juan,Yang Le,Zhu Yu2010 Northwestern Polytechnical University28807] [6] Qiu X M, Tang D L, Sun A P, Liu W D, Zeng X J 2007 Chin. Phys. B 16196 [7] Liao C En 1994Basic Technology of Microwave(Xi'an: Xidian University Press) (in Chinese) [Liaocheng En1994 Microwave technology base(Xi'an:Xi'an University of Electronic Science and Technology Press)] [8] Li S F, Li C R, Song C L 2013Fundamental Course of Optical Waveguide Theory, (Beijign: Publishing Hourse of Electronics Industry) (in Chinese) [Li Shufeng,Li Chengren,Song DynastyChang Lie2013Waveguide theory based tutorial(Beijing:Electronic Industry Press)] Physical Science Daily (2014) 154103 Acta Phys. Sin. Vol. 63, No. 15 Resonance experiment on a microwave resonator system* Shi Feng Yang Juan† Tang Ming-Jie Luo Li-Tao Wang Yu-Quan (College of Astronautics, Northwestern Polytechnic University, Xi'an 710072, China) (Received 9 January 2014; revised manuscript received 18 March 2014) Abstract A microwave resonator system is made, which has a tapered resonant cavity, a microwave source, and a transmission device. Because of the electromagnetic pressure gradient on the tapered resonant cavity, a net electromagnetic force along the axis of the cavity may be observed, which is needed to verify experimentally the use of the independent microwave resonator system. It is also needed to keep the independent microwave resonator system in resonating state, which is the important procedure to demonstrate the possibility of net electromagnetic force. Thus, a low-signal resonating experiment on the tapered resonant cavity combined with resonating parts is completed to accurately fi nd out the resonant frequency of 2.45 GHz and to analyze the in fl uence of temperature on the resonant state. Experimental result shows that the resonant frequency and quality factor of the independent microwave resonator system are 2.44895 GHz and 117495.08 respectively. When the temperature of the tapered resonant cavity wall rises, the resonant frequency will be decreased and the quality factor changed separately. Keywords: applied classical electromagnetism, electromagnetic wave propagation, microwave and radiowave instruments and equipment PACS:41.20.-q, 41.20.Jb, 07.57.-c DOI: 10.7498 / aps.63.154103 *Project supported by the National Natural Science Foundation of China (Grant No. 90716019). . † Corresponding author E-mail: yangjuan@nwpu.edu.cn 15410317