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As explained in the introductory section, direct-current (DC) machines are easier to analyze than their AC counterparts, although their actual construction is made rather complex by the need to have a commutator, which reverses the direction of currents and uxes to produce a net torque The objective of this section is to describe the major construction features and the operation of direct-current machines, as well as to develop simple circuit models that are useful in analyzing the performance of this class of machines Physical Structure of DC Machines A representative DC machine was depicted in Figure 178, with the magnetic poles clearly identi ed, for both the stator and the rotor Figure 1712 is a photograph of the same type of machine Note the salient pole construction of the stator and the slotted rotor As previously stated, the torque developed by the machine is a consequence of the magnetic forces between stator and rotor poles This torque is maximum when the angle between the rotor and stator poles is 90 Also, as you can see from the gure, in a DC machine the armature is usually on the rotor, and the eld winding is on the stator To keep this torque angle constant as the rotor spins on its shaft, a mechanical switch, called a commutator, is con gured so the current distribution in the rotor winding remains constant and therefore the rotor poles are consistently at 90 with respect to the xed stator poles In a DC machine, the magnetizing current is DC, so that there is no spatial alternation of the stator poles due to time-varying currents To understand the operation of the commutator, consider the simpli ed diagram of Figure 1713 In the gure, the brushes are xed, and the rotor revolves at an angular velocity m ; the instantaneous position of the rotor is given by the expression = m t.

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This chapter begins a sequence of nine chapters on the molecular structure of the genetic material, its replication, its expression, and the control of its expression. In this chapter, we look at the evidence that DNA is the genetic material, the chemistry of DNA, and the way in which DNA replicates, including the general enzymatic processes. We look rst at prokaryotic, then at eukaryotic, DNA replication. Note that we concentrate on the molecular structure of DNA because, generally, structure reveals function: molecules have shapes that de ne how they work.

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The commutator is xed to the rotor and is made up in this example of six segments that are made of electrically conducting material but are insulated from each other Further, the rotor windings are con gured so that they form six coils, connected to the commutator segments as shown in Figure 1713 As the commutator rotates counterclockwise, the rotor magnetic eld rotates with it up to = 30 At that point, the direction of the current changes in coils L3 and L6 as the brushes make contact with the next segment Now the direction of the magnetic eld is 30 As the commutator continues to rotate, the direction of the rotor eld will again change from 30 to +30 , and it will switch again

e wish to suggest a structure for the salt of deoxyribose nucleic acid (D.N.A.). This structure has novel features which are of considerable biological interest. A structure for nucleic acid has already been proposed by Pauling and Corey.1 They kindly made their manuscript available to us in advance of publication. Their model consists of three intertwined chains, with the phosphates near the bre axis, and the bases on the outside. In our opinion, this structure is unsatisfactory for two reasons: (1) We believe that the material which gives the X-ray diagrams is the salt, not the free acid. Without the acidic hydrogen atoms it is not clear what forces would hold the structure together, especially as the negatively charged phosphates near the axis will repel each other. (2) Some of the van der Waals distances appear to be too small. Another three-chain structure has also been suggested by Fraser (in the press). In his model the phosphates are on the outside and the bases on the inside, linked together by hydrogen bonds.This structure as described is rather ill-de ned, and for this reason we shall not comment on it. We wish to put forward a radically different structure for the salt of deoxyribose nucleic acid.This structure has two helical chains each coiled round the same axis (see diagram

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