Галерея 3156523

Галерея 3156523




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Галерея 3156523
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Cozy home on a nice sized lot that backs up to a greenbelt. Front and back yard are fully established yards with automatic sprinkler system. Home has 4 bedrooms and a roomy open concept living area. Only 2 miles from I 35 for quick access to work. Subdivision has an HOA park with playground and pool.
General
Price: $320,000 HOA FEE: $30/month HOA FEE FREQ.: Quarterly Taxes: $3,050 (2022) Status: Under Contract Type: Single Family MLS ID: 3156523 Updated: 3/8/2023 Added: 40 day(s) ago


Interior

Interior Features: Breakfast Bar, Granite Counters, Electric Dryer Hookup, Kitchen Island, No Interior Steps, Open Floorplan, Pantry, Primary Bedroom on Main, Recessed Lighting, Smart Home, Walk-In Closet(s), Washer Hookup Appliances: Dishwasher, Disposal, Dryer, Exhaust Fan, Microwave, Free-Standing Electric Range, Stainless Steel Appliance(s), Washer, Water Heater-Electric Flooring: Carpet, Tile
Rooms
Bathrooms
Total Bathrooms: 2 Full Bathrooms: 2 Bathroom 1: Full Bath, Main
Bedrooms
Total Bedrooms: 4 Bedrooms Main: 4
Other Rooms
Living Room: Smart Home, Main Kitchen: Breakfast Bar, GranCnt, Dining Area, Open to Family Room, Pantry, Main Dining Room: Recessed Lighting, Main Laundry: Inside, Laundry Room
Additional Information

Shared Amenities: Playground, Pool Security/Safety: Smoke Detector(s) Other Features: None
Exterior

Exterior Features: Exterior Steps, Private Yard Deck/Patio: Covered, Front Porch, Rear Porch
Parking

Garage: Yes Covered Spaces: 2 Total Spaces: 4 Parking Features: Attached, Driveway, Garage, Garage Faces Front
Location

Area: JA County: Williamson Subdivision: Schwertner Ranch Ph II Driving Directions: From Georgetown take I 35 North approximately 12 miles to Exit for CR 313E. Turn right on CR 313E. Go 2.3 miles to Schwertner Ranch entrance on the left. After entering the subdivision take the first right (Taggert). House is on the right. Direction Faces: West
School Information

Elem School District: Jarrell ISD Midd School District: Jarrell ISD High School District: Jarrell ISD Elementary School: Jarrell Middle School: Jarrell High School: Jarrell
Community

Association: Yes Assoc. Name: Real Manage Austin Assoc. Fees Include: Common Area Maintenance


Heating & Cooling

Cooling Type: Central Air, Electric Heating Type: Central
Utilities

Sewer: Municipal Utility District (MUD) Water: Municipal Utility District (MUD) Utility Description: Electricity Connected, Sewer Connected, Water Connected
Structural Information

Exterior Const.: Brick, Concrete, Frame, HardiPlank Type, Blown-In Insulation Foundation: Slab Roof: Composition Windows: Blinds, Insulated Windows, Screens, Vinyl Windows Disability Access: None Square Feet: 1,613 Living Area: 1,613 Sq. Ft. Year Built: 2021 Property Condition: Resale
Additional Structures

Other Structures: None
Lot Features

Property View: Neighborhood, Park/Greenbelt Lot Size (Acres): 0.1377 Lot Size (Sq. Ft.): 5,998.21 Lot Features: Back to Park/Greenbelt, Back Yard, Curbs, Front Yard, Sprinkler - Automatic Lot Description: Back to Park/Greenbelt, Back Yard, Curbs, Front Yard, Sprinkler - Automatic Fencing (Description): Back Yard, Privacy
Water Features

Water Front View: None
Financial Considerations

Lot Price Per Sq. Ft.: $53.35 Association Fee: $90 Assoc Fee Freq.: Quarterly Tax Amount: $3,050.53 Tax Year: 2022
Disclosures and Reports

Buyer’s Brokerage Compensation: 3% Documents Avail.: None Available Restrictions: Deed Restrictions Property ID: 11949002030027


School District: Jarrell Independent School District

1615 County Road 313, Jarrell, TX 76537
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560 Taggart Trl, Jarrell, TX 76537 (MLS# 3156523) is a
Single Family property with 4 bedrooms and 2 full bathrooms.
560 Taggart Trl is currently listed for $320,000 and was received on January 28, 2023.
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United States Patent 3,156,523 ELEMENT 95 AND METHOD OF PRODUCING SAKD ELENENT Glenn T. Seahorg, Chicago, Ill, assignor to the United States of America as represented by the United States Atomic Energy Commission No Drawing. Filed Aug. 23, 1946, Ser. No. 692,730 12 Claims. (Cl. 23-145) The present invention relates to a new transuranic element. More particularly it is concerned with the transuranic element having atomic number 95, now known as americium having the symbol Am, isotopes thereof, compositions containing the same, and methods of producing and purifying said element and compositions thereof.
The expression element 95 is used throughout this description to designate the element having atomic number 95. Reference herein to this element is to be understood as denoting the element generically whether singly or in combination, unless otherwise indicated by the context.
As far as is presently known two isotopes of americium have been synthesized in identifiable quantities, i.e., Am and Am The former isotope is an alpha emitter having a half life of 500 years, while the latter is a short-lived (17*18 hours half-life) beta emitter which is transformed relatively rapidly into element 96 known as curium and having the symbol Cm, an isotope of another new transuranic element and an alpha emitter having a half-life of about five months. The alpha particles emitted from this isotope have a range in air of 4.75 cm. A second isotope, Cm is produced by the bombardment of 94 with alpha particles. This isotope has a half-life of thirty days and is also an alpha emitter. The alpha particles produced thereby have a range of 5.0 cm. in air.
In accordance with the present invention, it has been found that these isotopes of element 95 can be produced in a variety of ways such as, for example, by bombarding plutonium produced in a -neutronic-reactor, which consists essentially of isotope 94 together with arelatively small concentration of isotope 94 Lwith subatomic particles, e.g., deuterons or neutrons. In preparing element 95 by the bombardment of plutonium with deuterons, for example, these subatomic particles should generally have energies of the order of at least mev. and preferably energies of 14 to '16 mev. or higher. The synthesis of element 95 in this manner is thought to involve at least a portion and very probably all of the nuclear reactions indicated below:
40 years 94239 12 95241 In general, it has been found that element 95 is most conveniently synthesized in a neutronic reactor operated at a relatively high power level (about 200 kw.) for extended period of time (approximately 100 days). A
suitable neutronic reactor which may be employed in the preparation of element 95 is described and claimed in err-pending application for United States Letters. Patent,
Serial No. 568,904 of Enrico Fermi and Leo Szilard, filed December 19, 1944, ,now Patent No. 2,708,656. In such reactors a fissionable isotope, such as U 5 in natural uranium, undergoes fission and releases fast neutrons in excess of the neutrons absorbed in the fission process.
The fast neutrons are slowed down to approximately thermal energies by impacts with a moderator such as graphite or deuterium oxide, and the resulting slow neutrons (energies of 0-03 electron volt) are then absorbed by U to produce further fission and by U to produce U which decays through 93 to 94 This selfsustaining chain reaction releases tremendous amounts of energy, primarily in the form of kinetic energy of the fission fragments. With such reactors the maximum reaction rate for steady state operation is determined by the maximum rate at which the heat of reaction can be removed. The rate of production of plutonium in such reactors may thus be equated, approximately, to the power output of the reactor, and amounts to about 0.9 gram of 94 per megawatt day when operating with sutlicient bombardment and aging times to permit total decay of 93 to 94 A portion of the 94 thus produced in the reactor under such conditions absorbs neutrons to form the isotope 94 In neutronic reactors operated under the general conditions of power level and time indicated above the absorption cross-section of 94 for the formation of 94 is rather large, amounting for thermal neutrons to nearly one-half the cross-section for the fission of 94 Thus plutonium produced in the above manner frequently contains as much as 2% of the .isotope 94 The latter isotope is an alpha emitter and also undergoes spontaneous fission to a slight extent (half-life for the process is 10 years). If this isotope is maintained in a neutronic reactor for a substantial period after its formation, it is transformed into the next heavier isotope which, in general, constitutes about .01 percent of the total plutonium produced under conditions of power level and time indicated above. As previously pointed out, 94 is a beta emitter and decays into 95 In a natural uranium pile, or neutronic reactor operating at such substantial powers and for substantial periods of time, the formation of element 95 (isotopes 95 and 95 and 96 is presumed to be synthesized in accordance with the following series of nuclear reactions:
I on] I 011 I 011 I m B- 13.. U239 N tat P zaa fission from which the plutonium was formed. Inasmuch as: the
decay of 94 to 95 occurs during as well as after the neutron bombardment period, the percentage of the latter in the transuranic fraction can be controlled by varying the time of bombardment, the time of aging subsequent to bombardment of uranium or both.
From an inspection of the above proposed nuclear reactions, it will be apparent that the formation of element 95 is dependent on the, concentration of 94 which is in turn dependent upon the amount of 94 produced. Also, While the desired concentration of element 95 in the transuranic fraction of the product may be obtained by sufiicient bombardment alone, it will be evident that a finite aging time will ensue before the separation of element 95 from the bombarded product can be effected. In the present description, therefore, it can be assumed that the bombarded product is always aged and that the concentration of element 95 in the transuranic fraction of the product is controlled by the total bombardment time plus P tan 9524i gm./ton t rug/ton of Uranium Uranium It will be apparent that element 95 can be synthesized at neutron fluxes considerably lower than neutrons/ cm. /sec.; however, at such intensities the formation of element 95 will be proportionately slower. In general, however, it will be found that neutron fluxes of at least 10 neutrons/cm. /sec. or higher are preferable.
Element 95 may be obtained from plutonium which has been previously isolated from uranium irradiated in a neutronic reactor of the type mentionedabove, in accordance with,'for example, the procedure set forth in copending application, Serial No. 637,484, filed December 27, 1945, by Glenn T. Seaborg et al. In accordance with this procedure, neutron bombarded uranium is dissolved in an aqueous solution of a suitable acid such as, for example, nitric acid and the resulting solution, which contains the plutonium in the tetravalent state and the uranium in the hexavalent or non-carriable state, is contacted With a' substantially insoluble, solid, finely divided compound which is a plutonium carrier. The carrier precipitate thus obtained containing plutonium is next separated from solution by any convenient means such as,- for example, centrifugation or filtration after which the product precipitate is again dissolved and the plutonium removed from solution by a carrier which is chemically distinct from the one first used. This procedure can be repeated if necessary. Also, a third carrier different inchemical composition from the first two mentioned may be utilized in a third precipitation. The advantage of these alternate carriers lies in the fact that certain impurities present in the process solution can be eliminated by employing a plutonium carrier that does not remove particular impurities with it. By proper selection and repeated application of such carriers, it will be seen that the separation of plutonium in the form of a relatively V I pure compound can be readily effected.
Metallic plutonium can be obtained means of high temperature reduction of a suitable halide thereof such as, for example, plutonium 'trifluoride, with a reactive metal such as lithium, sodium, barium, etc., in accordance with the procedure which is more fully described'in the aforementioned co-pend ing '=application, Serial No.
637,484, the d-isclosureof which is incorporated herein b'yfreference.
Element 95 present in the plutonium obtaihed in aclcord'anq with the procedure generally outlined above may be'isolatedtherefrom byfirst allowing the plutotion of the hydroxide-peroxide precipitation cycle denium to age for a desired period of time in metallic or.
solution form, for example, a salt solution such as a solution of plutonous nitrate, after which the bulk of the plutonium is separated from element by the addition of a soluble peroxide to the solution thereby converting plutonium to its substantially insoluble peroxide and leaving element 95 in solution as a soluble peroxide. The last traces of plutonium which amount to about 15% of th
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