Chapter 3 Part 19
By force of magnetic attraction it draws the hammer (J) towards it, and thus separates the two platinum points at (H). This separation interrupts the flow of the current, the core consequently loses its magnetism, and the hammer (J) returns by force of its spring (D) to its former position. Contact at (H) is thus restored, current passes as before in the primary, the core becomes again magnetised, and this cycle of events is repeated automatically as often as the succession of’ make ‘ and ‘ break’ at (H) will allow. The alternative path (dd) to the condenser (ee) will be dealt with later in reference to the suddenness of the break.
The secondary winding, which consists of many thousands of yards of very fine insulated copper wire, is not shewn in Fig. 41, but its position is within the bobbin (KK), and its endings are seen emerging at (FF), from which points con- nection is made to the X-ray tube.
Following the laws of induction, at each make of the primary current a momentary current is set up or induced in the secondary circuit in a direction opposite to that in the primary ; and at each break of the primary a momentary current is induced in the secondary in the same direction as the primary.
No related posts.
Tom Thym on October 19th 2009 in x-ray
