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RC4190M Datasheet(PDF) 19 Page - Raytheon Company |
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RC4190M Datasheet(HTML) 19 Page - Raytheon Company |
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19 / 25 page ![]() RC4190 PRODUCT SPECIFICATION 19 When the switch is the down position, the capacitor charges up to the battery voltage. The, when the switch is changed to the up position, the capacitor is put in series connection with the battery, and the doubled voltage is applied directly to the positive power supply lead of the RC4190. This voltage is enough to bias the junctions internal to the RC4190 and gets it started. Then, when the stepped up output voltage reaches a high enough value, diode D1 is forward biased and the out- put voltage takes over supplying power to the RC4190. The circuit is shown with component values for +5V output, but the circuit can be set up for other voltages. Electricity Versus Magnetism Electrically the inductor must meet just one requirement, but that requirement can be hard to satisfy. The inductor must exhibit the correct value of inductance (L, in Henrys) as the inductor current rises to its highest operating value (IMAX). This requirement can be met most simply by choosing a very large core and winding it until it reaches the correct induc- tance value, but that brute force technique wastes size, weight and money. A more efficient design technique must be used. Question: What happens if too small a core is used? First, one must understand how the inductor's magnetic field works. The magnetic circuit in the inductor is very similar to a simple resistive electrical circuit (see Figure 20). There is a magnetizing force (H, in oersteds), a flow of magnetism, or flux density (B, in Gauss), and resistance to the flux, called permeability (U, in Gauss per oersted). H is equivalent to voltage in the electrical model, flux density is like current flow, and permeability is like resistance (except for two important differences discussed on the following page). First Difference: Permeability, instead of being analogous to resistance, is actually more like conductance (1/R). As permeability increases, flux increases. Second Difference: Resistance is a linear function. As volt- age increases, current increases proportionally, and the resis- tance value stays the same. In a magnetic circuit the value of permeability varies as the applied magnetic force varies. This nonlinear characteristic is usually shown in graph form in ferrite core manufacturer's data sheets. See Figure 26. Figure 25. Electricity Versus Magnetism Figure 26. Typical Manufacturer’s Curve Showing Saturation Effect E I R E = I * R 65-3464-07 North Electrical Circuit Magentic Circuit South Flux H =B • 1 U 6000 5000 4000 3000 2000 1000 0 -0.5 0 0.5 1 2 2.5 3 5 7 9 H Oersteds +25 °C +85 °C +125 °C Stackpole Ceramag 24B Hysteresis Loop vs. Temperature |
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