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By using the following atomic masses : `._(92)^(238)U = 238.05079u`. `._(2)^(4)He = 4.00260u, ._(90)^(234)Th = 234.04363u`.
`._(1)^(1)H = 1.007834, ._(91)^(237)Pa = 237.065121u` (i) Calculate the energy released during the `alpha-`decay of `._(92)^(238)U`.
(ii) Show that `._(92)^(238)U` cannot spontaneously emit a proton.

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To solve the problem, we will follow these steps: ### Part (i): Calculate the energy released during the alpha decay of \(_{92}^{238}U\). 1. **Write the decay equation**: The alpha decay of Uranium-238 can be represented as: \[ _{92}^{238}U \rightarrow _{90}^{234}Th + _{2}^{4}He \] 2. **Identify the atomic masses**: - Mass of \(_{92}^{238}U = 238.05079 \, u\) - Mass of \(_{90}^{234}Th = 234.04363 \, u\) - Mass of \(_{2}^{4}He = 4.00260 \, u\) 3. **Calculate the mass defect (\(\Delta m\))**: \[ \Delta m = \text{mass of reactants} - \text{mass of products} \] \[ \Delta m = 238.05079 \, u - (234.04363 \, u + 4.00260 \, u) \] \[ \Delta m = 238.05079 \, u - 238.04623 \, u = 0.00456 \, u \] 4. **Convert the mass defect to energy**: Using the conversion factor \(1 \, u = 931.5 \, \text{MeV/c}^2\): \[ \text{Energy released} = \Delta m \times 931.5 \, \text{MeV/c}^2 \] \[ \text{Energy released} = 0.00456 \, u \times 931.5 \, \text{MeV/u} \approx 4.24764 \, \text{MeV} \] ### Part (ii): Show that \(_{92}^{238}U\) cannot spontaneously emit a proton. 1. **Write the decay equation for proton emission**: The reaction for proton emission can be represented as: \[ _{92}^{238}U \rightarrow _{91}^{237}Pa + _{1}^{1}H \] 2. **Identify the atomic masses**: - Mass of \(_{91}^{237}Pa = 237.065121 \, u\) - Mass of \(_{1}^{1}H = 1.007834 \, u\) 3. **Calculate the mass defect (\(\Delta m'\))**: \[ \Delta m' = \text{mass of reactants} - \text{mass of products} \] \[ \Delta m' = 238.05079 \, u - (237.065121 \, u + 1.007834 \, u) \] \[ \Delta m' = 238.05079 \, u - 238.072955 \, u = -0.022165 \, u \] 4. **Interpret the result**: Since \(\Delta m'\) is negative, it indicates that energy must be supplied to make this reaction occur, meaning that the reaction is not spontaneous. ### Summary of Results: - **Energy released during alpha decay**: \(4.24764 \, \text{MeV}\) - **Proton emission**: Not spontaneous due to negative mass defect.

To solve the problem, we will follow these steps: ### Part (i): Calculate the energy released during the alpha decay of \(_{92}^{238}U\). 1. **Write the decay equation**: The alpha decay of Uranium-238 can be represented as: \[ _{92}^{238}U \rightarrow _{90}^{234}Th + _{2}^{4}He ...
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We are given the following atomic masses: ._(92)^(238)U=238.05079u ._(2)^(4)He=4.00260u ._(90)^(234)Th=234.04363u ._(1)^(1)H=1.00783u ._(91)^(237)Pa=237.05121u Here the symbol Pa is for the element protactinium (Z=91)

The atomic mass of uranium ._(92)^(238)U is 238.0508 u , that of throium ._(90)^(234)Th is 234.0436 u and that of an alpha particle ._2^4He is 4.006 u , Determine the energy released when alpha-decay converts ._(92)^(238)U into ._(90)^(234)Th .

Show that ""_(92)^(238)U can not spontaneously emit a proton. Given: ""_(92)^(238)U = 238.05079u, ""_(91)^(237)Pa = 237.05121u ""_(1)^(1)H = 1.00783u

Write an equation of an alpha emission from U_(92)^(238)

The atomic mass of thorium ._(90)^(234)Th is 234.04359 u , while that of protactinium ._(91)^(234)Pa is 234.04330 u . Find the energy released when beta decay changes overset(234)(90)Th into Pa

How many alpha and beta -particles are emitted in the transformation ""_(92)^(238)U rarr ""_(92)^(234)U

Calculate the number of neutrons in the remaining atoms after the emission of an alpha particle from ._(92)U^(238) atom.

How many moles of helium are produced when 1 mole of ._(92)U^(238) disintegrate into ._(82)Pb^(206) ?

Alpha decay of ._(92)^(238)U forms ._(90)^(234)Th . What kind of decay from ._(90)^(234)Th produces ._(84)^(234)Ac ?

How many alpha and beta particles are emitted when uranium ._(92)^(238)U decays to lead ._(82)^(206)Pb ?

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