Gouy's method of magnetic susceptibility

Bsc physics honors solid state practical lab manual gouys method.

1. Solid state physics- Gouy method Practical ppt By Pratishtha

2. Aim - To de termine the magnetic susceptibility of a solid(Gouy’s method). Apparatus- An electromagnet with power supply , a sensitive balance , solid object in shape of a long cylinder ,gauss-meter and fractional weights Theory-(Gouy’s method): - This met hod depends on the force exerted on a body placed in a non homogenous mag netic field is obtained by measuring the apparent gain or loss in sample weight. The variable magnetic field is provided by an electromagnet with wedge shaped pole pieces.The field of the magnet varies rapidly along the vertical direction, due to the wedging of the pole pieces.Thus, the force on the specimen is vertical. In this experiment the influence of the earth's field is neglected.

3. Sample material

4. There is a hol e in the box through which the specimen hangs o ut. It is hung in the field between the pole pieces of t he magnet in such a way that its lower end is in a homogeneous magnetic field H and the upper end is in a much weaker field . Let in absence of the magnetic field weight of sample= m Let in the presence of magnetic field the weight of sample= m 1 Force on acting sample F=Δmg= (m 1 -m )g ------(1) We now derive an expression for the force applied by the magnet on the sample. A substance’s magnetic permeability is given by: u= u (1+✘) ✘= magnetic susceptibility. u = 4𝞹*10 -7 Wb/A.m We may find the difference in magnetic potential energy per unit volume between a substance of magnetic permeability u and the displaced medium (in our case, air, which has the permeability of free space) :

5. Δ(U/V)= (H 2 /2 u ) Air -( H 2 /2 u) sample = H 2 / 2u -( H 2 /2 u (1+ ✘ )) = ✘ H 2 /2 u (1+ ✘ ) { ✘=M/H} the magnetic susceptibility is significantly smaller than 1, ✘<<1 So (1+ ✘ )≅ 1 Δ(U/V)= ✘ H 2 /2 u Let us now consider a gradient in the field along the z-direction (upwards direction), as there is in the case of this experiment. If we assume that the magnetic susceptibility is constant throughout the sample, the force per unit volume f experienced by the sample is given by: f = -∂U/∂Z = - - - - A

6. Using Eq. A, we can then integrate over the length (with a constant cross-sectional area A) to find the total force on the sample by the magnetic field. Here, we will simply denote the top and the bottom z-values of the sample as “top” and “bottom” where A is the cross-sectional area of the sample and H is a measure of magnetic field at the top and bottom of the sample, respectively H top and H bottom are the measured magnetic fields at the top and bottom of the sample. If the length of the sample is sufficiently long, Htop may be treated as zero and H bottom may be generalized to simply H. Thus, Eq. A can be simplified. ------(B)

7. From equation (1) F=Δmg From equation (1) and (B) ✘= 2 u Δmg/AH Procedure- (i) connect the electromagnet with power supply. (ii) The specimen the shape of a rod is connected to one arm of a sensitive balance and hung vertically such that its lower end is in between the two pole pieces and the upper end outside the pole pieces. (iii)Put the weight in the other arm of the balance so as to bring its needle in the centre. In case of a digital weighing machine a knob is provided for the purpose and the mass is directly given by the machine. Note down the mass M of the rod. (iv) Switch on the field H and add weights in the pan to bring the balance needle at the centre. Note down the mass M 1 of the rod in the presence of the magnetic field. Then (M1-M0) gives the mass required to counter balance the effect of the magnetic field. Measure the field using a gauss-meter.

8. Final point (v) Change the field by varying the current in the power-supply of the electro magnet. Note down the magnetic field B and the corresponding mass M 1 of the rod. Take 5-6 such readings. (vi)Measure the area of cross-section of the sample with a suitable instrument. (vii)Plot a graph between H along x-axis and Δm along y-axis. ✘ =( 2 u g/A)* slope m(kg) H 2 (tesla)

9. All material can be classified by value of magnetic susceptibility into 3 groups- Diamagnetic -1< ✘ < 0 (repelled by magnetic f) Paramagnetic 0< ✘ << 1 (weakly attracted) Ferromagnetic ✘>> 1 (strongly attracted) Precautions and source of error-- (i)The pole pieces of the electromagnetic should be wedge shaped with enough spacing so that the field may be uniform. (ii)The current in the electromagnet should not be passed for long time. (iii) The balance should be very sensitive preferably a digital balance and should be enclosed in a box so that the weighing is not affected by the air. iv). The specimen should be freely suspended with no mechanical restraint from the balance.

10. Weak points- Gouy's method is a simple but not a sufficiently accurate one. This is because the force is weak even in strong fields because of the low values of susceptibilities of dia and paramagnetic substances. To produce a force equivalent to 1 gwt, the field required will be of the order of 10 gauss. Other methods i) faraday’s method ii) induction method iii) Quink’s tube method