Magnetic tape having characterized back coating layer

Patent metadata

Field	Value
Publication number	US-10424330-B2
Application number	US-201815900164-A
Country	US
Kind code	B2
Filing date	Feb 20, 2018
Priority date	Feb 20, 2017
Publication date	Sep 24, 2019
Grant date	Sep 24, 2019

Abstract

A magnetic tape includes a back coating layer having a thickness less than or equal to 0.30 μm and containing fatty acid ester. The logarithmic decrement acquired by a pendulum viscoelasticity test performed regarding the surface of the back coating layer is less than or equal to 0.060. The full width at half maximum of spacing distribution measured by optical interferometry regarding the surface of the back coating layer before and after performing a vacuum heating with respect to the magnetic tape is respectively greater than 0 nm and less than or equal to 10.0 nm, and the difference between the spacing measured by optical interferometry regarding the surface of the back coating layer after performing the vacuum heating and the spacing measured before performing the vacuum heating is greater than 0 nm and less than or equal to 8.0 nm.

First claim

What is claimed is:

1. A magnetic tape comprising:
a non-magnetic support;
a magnetic layer including ferromagnetic powder and a binding agent on one surface side of the non-magnetic support; and
a back coating layer including non-magnetic powder and a binding agent on the other surface side of the non-magnetic support,
wherein the thickness of the back coating layer is equal to or smaller than 0.30 μm,
the back coating layer includes fatty acid ester,
the logarithmic decrement acquired by a pendulum viscoelasticity test performed regarding the surface of the back coating layer is equal to or smaller than 0.060,
the full width at half maximum of spacing distribution measured by optical interferometry regarding the surface of the back coating layer before performing a vacuum heating with respect to the magnetic tape is greater than 0 nm and equal to or smaller than 10.0 nm,
the full width at half maximum of spacing distribution measured by optical interferometry regarding the surface of the back coating layer after performing the vacuum heating with respect to the magnetic tape is greater than 0 nm and equal to or smaller than 10.0 nm,
the difference S after −S before between a spacing S uer measured by optical interferometry regarding the surface of the back coating layer after performing the vacuum heating with respect to the magnetic tape and a spacing S before measured by optical interferometry regarding the surface of the back coating layer before performing the vacuum heating with respect to the magnetic tape is greater than 0 nm and equal to or smaller than 8.0 nm, and
the logarithmic decrement on the back coating layer side is determined by the following method:
securing a measurement sample of the magnetic tape with the measurement surface, which is the surface on the back coating layer side, facing upward on a substrate in a pendulum viscoelasticity tester;
disposing a columnar cylinder edge which is 4 mm in diameter and equipped with a pendulum 13 g in weight on the measurement surface of the measurement sample such that the long axis direction of the columnar cylinder edge runs parallel to the longitudinal direction of the measurement sample;
raising the surface temperature of the substrate on which the measurement sample has been positioned at a rate of less than or equal to 5° C./min up to 80° C.;
inducing initial oscillation of the pendulum;
monitoring the displacement of the pendulum while it is oscillating to obtain a displacement-time curve for a measurement interval of greater than or equal to 10 minutes; and
obtaining the logarithmic decrement Δ from the following equation:

Δ
=

ln
⁡

(

A
1

A
2

)

+

ln
⁡

(

A
2

A
3

)

+

⁢

…
⁢

⁢

ln
⁡

(

A
n

A

n
+
1

)

n

wherein the interval from one minimum displacement to the next minimum displacement is adopted as one wave period; the number of waves contained in the displacement-time curve during one measurement interval is denoted by n, the difference between the minimum displacement and the maximum displacement of the n th wave is denoted by An, and the logarithmic decrement is calculated using the difference between the next minimum displacement and maximum displacement of the n th wave (A n+1 in the above equation).

2. The magnetic tape according to claim 1 ,
wherein the logarithmic decrement is 0.010 to 0.060.

3. The magnetic tape according to claim 1 ,
wherein the thickness of the back coating layer is 0.10 μm to 0.30 μm.

4. The magnetic tape according to claim 1 ,
wherein the full width at half maximum of spacing distribution measured by optical interferometry regarding the surface of the back coating layer before performing a vacuum heating with respect to the magnetic tape is greater than 0 nm and equal to or smaller than 8.0 nm.

5. The magnetic tape according to claim 1 ,
wherein the full width at half maximum of spacing distribution measured by optical interferometry regarding the surface of the back coating layer after performing the vacuum heating with respect to the magnetic tape is greater than 0 nm and equal to or smaller than 8.0 nm.

6. The magnetic tape according to claim 1 ,
wherein the difference S after −S before is greater than 0 nm and equal to or smaller than 6.0 nm.

7. The magnetic tape according to claim 1 ,
wherein the logarithmic decrement is 0.010 to 0.060,
the thickness of the back coating layer is 0.10 μm to 0.30 μm,
the full width at half maximum of spacing distribution measured by optical interferometry regarding the surface of the back coating layer before performing a vacuum heating with respect to the magnetic tape is greater than 0 nm and equal to or smaller than 8.0 nm,
the full width at half maximum of spacing distribution measured by optical interferometry regarding the surface of the back coating layer after performing the vacuum heating with respect to the magnetic tape is greater than 0 nm and equal to or smaller than 8.0 nm, and
the full width at half maximum of spacing distribution measured by optical interferometry regarding the surface of the back coating layer after performing the vacuum heating with respect to the magnetic tape is greater than 0 nm and equal to or smaller than 8.0 nm.

8. The magnetic tape according to claim 1 ,
wherein the non-magnetic powder included in the back coating layer is one or more kinds of non-magnetic powder selected from the group consisting of inorganic powder and carbon black.

9. The magnetic tape according to claim 8 ,
wherein the content of the inorganic powder in the back coating layer is greater than 50.0 parts by mass and equal to or smaller than 100.0 parts by mass with respect to 100.0 parts by mass of the total amount of the non-magnetic powder included in the back coating layer.

Assignees

• Fujifilm Corp

Inventors

• Kasada Norihito

Classifications

• G11B5/735

  characterised by the back layer {(magnetic recording media substrates G11B5/739)} · CPC title

• G11B5/78

  Tape carriers · CPC title

• G11B5/708

  characterised by addition of non-magnetic particles to the layer · CPC title

• G11B5/712 Primary

  characterised by the surface treatment or coating of magnetic particles · CPC title

• G11B5/7356 Primary

  comprising non-magnetic particles in the back layer, e.g. particles of TiO2, ZnO or SiO2 · CPC title