Full Scale Drift Tube Magnet Report Page: 12
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found to explain Um difference betveen the model and full scale measure-
the full scale measurements art well vithn this wl—i e
For magnets 5 through 8 the force on each vindng of the magnet vas
total forco is determined by ntegrating over the entre volume of the
type of measurement involved.
From Um —our—ato made on 1-2, 2-3, 5 through 8 it — concluded
that the —del —a our—an to are aocurate within 15 pore—t and therefore
it was no t considered advisable to take the —e— a ary time for direct measure-
menta — magnets 3-4, 45.
The values for the —ter flow war a determined from naaaw—anta —do
reduced to the 64 pounds pr——ra drop that will be available at the pl—t
Ing that the flow rate varies directly — the aquare of the
alto by
Pover vas determned — the product of voltage and cur rout
across the magnet windingo.
The resistance and water flow —
values for —tor proaoura, power, resistance, and —ter flow are listed
in Table I.
■
I
•e
• woo
*o S 5* ;;
woo a ♦ • o
• • • • ==
calculated from the mearrements of radial components of the field. The
te were dfrect, 411 the above
at 70 pounds pressure drop across Umi magnet terminals. These values were
me
• o
" 2 :
a e e • •
=s • eea 0 •
UCRL—1885
ments in thia case. However, since the allovable force la around 6000 pounds
ooll. Thia method of determining for— la only valid where the —o—t
of steel in the presence of the coil la small. Therefore thin technique
could only be need — magnets 5 through 8. The greatest variation bet—on
calculated waaaur—ante — the full scale magnet a— direct nodel measure-
ments vas 15 pore—t. Thio vas considered to be good agra —t for the
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Sewell, D. & Parmentier, H. Full Scale Drift Tube Magnet Report, report, July 1952; Berkeley, California. (https://digital.library.unt.edu/ark:/67531/metadc1255505/m1/12/: accessed July 18, 2024), University of North Texas Libraries, UNT Digital Library, https://digital.library.unt.edu; crediting UNT Libraries Government Documents Department.