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$$Density=45\ Kg/m^3$$ $$Valume=6\ m^3$$

$$u =270\ Kg$$

$$m = pV$$
Where:

p = density

m = mass

V = volume

$$density= 45\ m/s$$ $$mass= 6\ m/s$$

$$valume= 0.13333\ m^3 $$

$$V = \dfrac{m}{p}$$
Where:

p = density

m = mass

V = volume

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In Physics, the thickness of the substance is characterized as the connection between the mass of the substance and the space involved by the substance, typically the volume. It is characterized as the mass per unit volume. Numerically, the thickness of the substance is characterized as the mass partitioned by the volume. Thickness is a concentrated property, and the recipe to compute the thickness is given as follow:

**Thickness (D) = Mass (M)/Volume(V) **

The SI unit to gauge thickness is kilogram per cubic meter (Kg/m3).

where:

**ρ** is the thickness

**m** is the mass

**V** is the volume

The count of thickness is very direct. Be that as it may, it is critical to give uncommon consideration to the units utilized for thickness computations. There are various approaches to communicate thickness, and not utilizing or changing over into the legitimate units will bring about an inaccurate worth. It is helpful to painstakingly work out whatever qualities are being worked with, including units, and perform a dimensional examination to guarantee that the eventual outcome has units of mass/volume. Note that thickness is additionally influenced by pressing factor and temperature. On account of solids and fluids, change in thickness is commonly low. Be that as it may, when with respect to gases, the thickness is to a great extent influenced by temperature and pressing factors. An expansion in pressing factor diminishes volume and consistently expands thickness. Expansions in temperature will, in general, diminish thickness since the volume will for the most part increment. There are special cases be that as it may, for example, water's thickness expanding somewhere in the range of 0°C and 4°C.

The following is a table of units where the thickness is usually communicated, just as the densities of some basic materials.

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