1. Introduction
Microwaves are maybe, one of the greatest discovers of the 20’th century. With a vavelenght between 30 cm and 3 mm and a power between 1 mW and 500 KW are practically used in all fields from medicine to industry. Microwave thermal and chemical tratments are well known for the high efficiency, with 3 to 1000 times greatest then conventional process because of direct energy transfer into materials and selectivity compounds heating following dielectric permittivity parameters of the materials involved in reaction or in the treatment (equation 1):
where: – e’ is the real part of the permittivity, which characterize the amount of microwave reactive power changed with material (without absorption);
– e’’eff is the imaginary part of the permittivity, which characterize the microwave global absorption’s in the material.
The permittivity is a function of the material temperature and of the microwave frequency. In the general case, the permittivity is a tensor which depends on the homogeneity and anisotropy of the materials. The microwave power absorbed in the material, assuming that all microwave power is transformed in warmth, is (equation 2):
Any microwave oven is a multimodal microwave cavity in which the incident power ( usual 700W to 70KW at 2.45 GHz ) has a particular distribution . If the probe to be treated has a great volume ( like drying foods in foodstuff industry or ceramic materials microwave drier ), this multimodal cavity is suitable for a treatment because many parts of the local power distribution are intersecting the probe volume. The user must have a total control for the microwave radiation like: modifying continuously the output power in a large range ( not only the output energy used in almost all home-appliance ovens ) and controlling precisely the treatment period.
We present here, briefly, our design concerning a 5KW magnetron oven with an effective volume of 1 cubic meter, based on continuous wave CK 101 magnetron and driven by a flash microcontroller PIC16F877.
2.The concept
In fig.1 is shown the typical structure for our high power microwave oven:
Fig.1 Typical high power structure of a microwave oven –
The magnetron ( microwave power generator ) is supplied through an anodic transformer ( T1-6KV/1A ) and a two steps filament transformer ( T2-7.5V/42A and 5.5V/36A ). The magnetic field of the magnetron is produced in two coils ( L1 supplied from a PWM based constant current source, with max.10A and 20V voltage swing and L2 supplied by a feedback anodic current ).
All supplying algorithm are supervised by microcontroller board (4) with a simple interface user (6) consisting in four functional buttons ( the same buttons have different functions displayed on the second line of the LCD as the program flow chart required) and a large LCD display. Because the high anodic temperature ( 150 C ), a cooling system ( with cold water and air flow ) is required. Both the water flow command and air flow presence are supervised by the microcontroller board using an anodic temperature measurement. All other parameters like door status ( open or closed ), cooling water pressure, treatment period and output microwave power are also under microcontroller control.
Read more: MICROCONTROLLER BASED INTERFACE UNIT FOR 5KW MICROWAVE OVEN