Home
Class 12
CHEMISTRY
For a 3s-orbital Phi(3s)=(1)/(asqrt(3)...

For a 3s-orbital
`Phi(3s)=(1)/(asqrt(3))((1)/(a_(0)))^(3//2)(6-6sigma+sigma^(2))in^(-sigma//2)`
where `sigma=(2rZ)/(3a_(sigma))`
What is the maximum radial distance of node from nucleus?

A

`((3+sqrt(3))a_(sigma))/(Z)`

B

`(a_(sigma))/(Z)`

C

`(3)/(2)((3+sqrt(3))a_(sigma))/(Z)`

D

`(3a_(sigma))/(Z)`

Text Solution

AI Generated Solution

The correct Answer is:
To find the maximum radial distance of the node from the nucleus for a 3s orbital, we will follow these steps: ### Step-by-Step Solution: 1. **Understand the Wave Function**: The wave function for a 3s orbital is given by: \[ \Phi(3s) = \frac{1}{a\sqrt{3}} \left(\frac{1}{a_0}\right)^{3/2} (6 - 6\sigma + \sigma^2) e^{-\sigma/2} \] where \(\sigma = \frac{2rZ}{3a_\sigma}\). 2. **Set the Wave Function to Zero**: To find the nodes, we need to set the wave function equal to zero: \[ 6 - 6\sigma + \sigma^2 = 0 \] 3. **Rearranging the Equation**: Rearranging the quadratic equation gives us: \[ \sigma^2 - 6\sigma + 6 = 0 \] 4. **Using the Quadratic Formula**: We can solve for \(\sigma\) using the quadratic formula: \[ \sigma = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a} \] Here, \(a = 1\), \(b = -6\), and \(c = 6\): \[ \sigma = \frac{6 \pm \sqrt{(-6)^2 - 4 \cdot 1 \cdot 6}}{2 \cdot 1} \] \[ \sigma = \frac{6 \pm \sqrt{36 - 24}}{2} \] \[ \sigma = \frac{6 \pm \sqrt{12}}{2} \] \[ \sigma = \frac{6 \pm 2\sqrt{3}}{2} \] \[ \sigma = 3 \pm \sqrt{3} \] 5. **Choosing the Positive Root**: We take the positive root for \(\sigma\): \[ \sigma = 3 + \sqrt{3} \] 6. **Relate \(\sigma\) to Radial Distance \(r\)**: Recall that: \[ \sigma = \frac{2rZ}{3a_\sigma} \] Rearranging gives: \[ r = \frac{3a_\sigma \sigma}{2Z} \] 7. **Substituting \(\sigma\)**: Substitute \(\sigma = 3 + \sqrt{3}\) into the equation for \(r\): \[ r = \frac{3a_\sigma (3 + \sqrt{3})}{2Z} \] ### Final Answer: The maximum radial distance of the node from the nucleus is: \[ r = \frac{3a_\sigma (3 + \sqrt{3})}{2Z} \]

To find the maximum radial distance of the node from the nucleus for a 3s orbital, we will follow these steps: ### Step-by-Step Solution: 1. **Understand the Wave Function**: The wave function for a 3s orbital is given by: \[ \Phi(3s) = \frac{1}{a\sqrt{3}} \left(\frac{1}{a_0}\right)^{3/2} (6 - 6\sigma + \sigma^2) e^{-\sigma/2} \] ...
Doubtnut Promotions Banner Mobile Dark
|

Topper's Solved these Questions

  • STOICHIOMETRY AND BALANCING REDOX REACTION

    FIITJEE|Exercise SINGLE INTEGER ANSWER TYPE QUESTIONS|5 Videos
  • THERMODYNAMICS AND THERMOCHEMISTRY

    FIITJEE|Exercise SINGLE INTEGER ANSWER TYPE QUESTIONS|5 Videos

Similar Questions

Explore conceptually related problems

For a 3s - orbital, value of Phi is given by following realation: Psi(3s)=(1)/(9sqrt(3))((1)/(a_(0)))^(3//2)(6-6sigma+sigma^(2))e^(-sigma//2)," where " sigma=(2r.Z)/(3a_(0)) What is the maximum radial distance of node from nucleus?

For an orbital in B^(+4) radial function is : R(r ) = (1)/(9sqrt(6))((z)/(a_(0)))^((3)/(4))(4-sigma)sigma e^(-sigma//2 where sigma = (Zr)/(a_(0)) and a_(0)=0.529Å,Z = atomic number, r= radial distance from nucleus. The radial node of orbital is at distance from nucleous.

Knowledge Check

  • According to qauntum mechanical model of H-like species, and electron can be represented by a wave function (psi) which contain all dynamic information about the electron. The nature of wave function depends on the type of the orbital to which the electron belongs. For an orbital psi=[sqrt(2)/(81sqrt(3pi))]((1)/(a_(0)))^(3//2)(27-18sigma+2sigma^(2))e^((sigma)/(3)) Where, sigma =((Zr)/(a_(0))),r = radial distance from nucleous, a_(0)=52.9"pm" The number of radial and angular nodes possible for the orbital given above are respectively

    A
    zero,zero
    B
    `0,2`
    C
    `2,0`
    D
    `2,1`
  • According to qauntum mechanical model of H-like species, and electron can be represented by a wave function (psi) which contain all dynamic information about the electron. The nature of wave function depends on the type of the orbital to which the electron belongs. For an orbital psi=[sqrt(2)/(81sqrt(3pi))]((1)/(a_(0)))^(3//2)(27-18sigma+2sigma^(2))e^((sigma)/(3)) Where, sigma =((Zr)/(a_(0))),r = radial distance from nucleous, a_(0)=52.9pm Which of the following represents the position of one of the radial nodes?

    A
    `r=(1)/(2)(3+sqrt(3))a_(0)`
    B
    `r=(1)/(2)(3-sqrt(3))a_(0)`
    C
    `r=(3)/(2)(3-sqrt(6))a_(0)`
    D
    `r=(3)/(2)(3+sqrt(3))a_(0)`
  • According to qauntum mechanical model of H-like species, and electron can be represented by a wave function (psi) which contain all dynamic information about the electron. The nature of wave function depends on the type of the orbital to which the electron belongs. For an orbital psi=[sqrt(2)/(81sqrt(3pi))]((1)/(a_(0)))^(3//2)(27-18sigma+2sigma^(2))e^((sigma)/(3)) Where, sigma =((Zr)/(a_(0))),r = radial distance from nucleous, a_(0)=52.9pm The orbital could possibly be

    A
    `4s`
    B
    `4p`
    C
    `3s`
    D
    `3p`
  • Similar Questions

    Explore conceptually related problems

    For H-atom wave function for a particulaonstate is: Psi=(1)/(81sqrt(3pi))((1)/(a_(0)))^(3//2) (sigma^(2)-10sigma+25)e Where sigma=r//a_(0) and a_(0) is Bohr's radius (0.53overset(@)A) . Then distance of farthest radius mode is approximately.

    Calcuted the distance of spherical nodes for '3s' orbital from nucleus ? R_(3s)=(1)/(9sqrt3a_(0)^(3//2))(6-6sigma+sigma^(2))e^((sigma)/(2)) Where sigma=(2r)/(na_(0))

    Given the H- atom R_(n,l) = (1)/(9sqrt(3))((1)/(a_(o)))^(3//2)(6 - 6sigma + sigma^(2))e^(-sigma//2) where sigma = (2Zr)/(na_(o)), a_(o) = 0.53Å Select the correct statement for the given orbital ?

    The Schrodinger wave equation for hydrogen atom of 4s- orbital is given by : Psi (r) = (1)/(16sqrt4)((1)/(a_(0)))^(3//2)[(sigma^(2) - 1)(sigma^(2) - 8 sigma + 12)]e^(-sigma//2) where a_(0) = 1^(st) Bohr radius and sigma = (2r)/(a_(0)) . The distance from the nucleus where there will be no radial node will be :

    The wave function of 3s and 3p_(z) orbitals are given by : Psi_(3s) = 1/(9sqrt3) ((1)/(4pi))^(1//2) ((Z)/(sigma_(0)))^(3//2)(6=6sigma+sigma)e^(-sigma//2) Psi_(3s_(z))=1/(9sqrt6)((3)/(4pi))^(1//2)((Z)/(sigma_(0)))^(3//2)(4-sigma)sigmae^(-sigma//2)cos0, sigma=(2Zr)/(nalpha_(0)) where alpha_(0)=1st Bohr radius , Z= charge number of nucleus, r= distance from nucleus. From this we can conclude: